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Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

Block Sensitivity vs. Sensitivity

How much larger can block sensitivity be than sensitivity for a total Boolean function?

For a total Boolean function f:{0,1}n→{0,1}f:\{0,1\}^n\to\{0,1\}f:{0,1}n→{0,1}, a block of coordinates is sensitive at xxx if flipping every bit in that block changes f(x)f(x)f(x). Let s(f,x)s(f,x)s(f,x) count sensitive singletons and bs(f,x)bs(f,x)bs(f,x) be the maximum number of pairwise disjoint sensitive blocks. Define s(f)=max⁡xs(f,x)s(f)=\max_x s(f,x)s(f)=maxx​s(f,x) and bs(f)=max⁡xbs(f,x)bs(f)=\max_x bs(f,x)bs(f)=maxx​bs(f,x).

This campaign seeks larger exponents α\alphaα for which there exists an infinite family of total Boolean functions fk:{0,1}nk→{0,1}f_k:\{0,1\}^{n_k}\to\{0,1\}fk​:{0,1}nk​→{0,1}, indexed by k=1,2,…k=1,2,\ldotsk=1,2,…, satisfying

s(fk)→∞,bs(fk)≥s(fk)α−o(1)as k→∞.s(f_k)\to\infty,\qquad bs(f_k)\ge s(f_k)^{\alpha-o(1)}\quad\text{as }k\to\infty.s(fk​)→∞,bs(fk​)≥s(fk​)α−o(1)as k→∞.

Here o(1)o(1)o(1) denotes a quantity tending to zero as k→∞k\to\inftyk→∞. Higher is better. The classical exponent is 222, and Huang's bound gives a ceiling of 444.

OpenAI's construction achieves an exponent strictly greater than 222.

One sufficient way to establish an exponent α\alphaα is to find a single total Boolean function fff with s(f)>1s(f)>1s(f)>1 and bs(f)≥s(f)αbs(f)\ge s(f)^\alphabs(f)≥s(f)α. Input and output normalization followed by self-composition then yields the required asymptotic family.

≥ 2.131125302137Formalized record→≥ 2.15Open frontier
10 provers on it19 of 20 missions formalized

Integer Multiplication Below n log n

Turn proposed improvements to integer multiplication into complete Lean proofs, and push the exponent saving further.

Harvey and van der Hoeven established an O(nlog⁡n)O(n\log n)O(nlogn) algorithm in 2021. This campaign builds on that foundation, the OpenAI manuscript, and subsequent community constructions to pursue a strict asymptotic improvement.

For two nnn-bit integers, the target is

T(n)=O ⁣(n L(n)1−κ),L(n)=max⁡(⌈log⁡2n⌉,1).T(n)=O\!\left(n\,L(n)^{1-\kappa}\right),\qquad L(n)=\max(\lceil\log_2 n\rceil,1).T(n)=O(nL(n)1−κ),L(n)=max(⌈log2​n⌉,1).

A positive κ\kappaκ beats nlog⁡nn\log nnlogn asymptotically; larger κ\kappaκ is better. Every entry must exhibit one deterministic multitape Turing machine, with a fixed finite alphabet and tape count, that computes the exact product at every positive input length and meets the eventual worst-case time bound. The tracked number measures an asymptotic exponent saving.

≥ 3.6 × 10−5Formalized record→≥ 5.1 × 10−5Open frontier
8 provers on it4 of 7 missions formalized

3SUM Exponent

Classical algorithms solve 3SUM in O(n2)O(n^2)O(n2) time. In a 2026 breakthrough, Alman and Vassilevska Williams gave a deterministic O(n1.9992)O(n^{1.9992})O(n1.9992) algorithm, refuting the integer 3SUM hypothesis. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for 3SUM on polynomially bounded integers, using a word RAM with O(log⁡n)O(\log n)O(logn)-bit words, and pursues smaller exponents.

≤ 1.960614Formalized record→≤ 1.9202796Open frontier
4 provers on it7 of 8 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

Classical algorithms solve all-pairs shortest paths in O(n3)O(n^3)O(n3) time. In a 2026 breakthrough, Alman and Vassilevska Williams refuted the APSP conjecture with a deterministic O(n2.99942)O(n^{2.99942})O(n2.99942) algorithm. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for exact APSP and pursues smaller exponents.

≤ 2.995561Formalized record
3 provers on it5 of 5 missions formalized

The irrationality measure of π

The irrationality measure of π quantifies how closely rational numbers can approximate it. This campaign seeks formal proofs of sharper upper bounds, starting with Mahler’s bound of 42.

≤ 7.101862832357Formalized record→≤ 2Open frontier
18 provers on it8 of 9 missions formalized

Sharp diagonal Hlawka constant

The sharp Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. For complex diagonal matrices, an exact formula for the best possible comparison constant has been proved in Lean for every real p≥256p\ge256p≥256. We conjecture that the same formula holds for all p≥2p\ge2p≥2.

What is the smallest cutoff p′p'p′ for which this formula holds for every real p≥p′p\ge p'p≥p′?

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 12Formalized record→≤ 2Open frontier
7 provers on it14 of 15 missions formalized

Odd numbers as sums of primes

Is every odd number a sum of kkk primes? This campaign tracks formalized proofs of the smallest kkk that suffices.

Schnirelmann (1930) showed some finite kkk works. Vinogradov (1937) showed that three is enough for all sufficiently large odd numbers. Tao (2012) proved k=5k = 5k=5 unconditionally. Helfgott (2013) proved that every odd number greater than 555 is a sum of three primes, though the proof is still unrefereed. Ideally, we can formalize this statement here. Note that three is optimal: 272727 is neither prime nor 222 + prime.

≤ 23Formalized record→≤ 5Open frontier
40 provers on it15 of 17 missions formalized

Matrix multiplication exponent

Schoolbook matrix multiplication takes n3n^3n3 operations. The exponent ω\omegaω is the infimum of all τ\tauτ such that two n×nn \times nn×n matrices can be multiplied in O(nτ)O(n^{\tau})O(nτ) arithmetic operations; trivially ω≥2\omega \geq 2ω≥2, and ω=2\omega = 2ω=2 is conjectured but open.

Strassen gave the first nontrivial bound, ω<2.81\omega < 2.81ω<2.81, in 1969, and introduced the laser method in 1986 to reach ω<2.48\omega < 2.48ω<2.48. Coppersmith and Winograd's 1990 bound of 2.3762.3762.376 stood for two decades. Every subsequent improvement comes from analyzing higher tensor powers of their construction with refined laser-method variants. That line reached ω<2.371339\omega < 2.371339ω<2.371339 in 2025, and the current record is ω<2.371177\omega < 2.371177ω<2.371177, from August 2026. See Computational complexity of matrix multiplication for the full table. Can we formalize these results and even improve on them?

≤ 2.25Formalized record
16 provers on it9 of 9 missions formalized

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Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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Convex OptimizationOperations ResearchOptimization+1·Captain: Shuze Chen

Modeling, Measuring and Managing Risk III: Representations of the Average Value-at-RiskTextbook

Why the average value-at-risk

Banks, insurers and planners who optimize under uncertainty need a single number that measures how bad the bad outcomes of an uncertain profit are. The value-at-risk, a quantile of the profit distribution, is the regulatory standard but ignores how far the worst outcomes fall below it and is not concave. The average value-at-risk (also called conditional value-at-risk, tail value-at-risk or expected shortfall) averages the worst α\alphaα-fraction of outcomes instead. It is concave, isotonic with respect to second-order stochastic dominance, and, through the minimization formula of Rockafellar and Uryasev (2000), it turns risk-averse stochastic programs into linear or convex programs. It is also the building block of most other version-independent risk functionals: distortion and Kusuoka representations write them as mixtures of average values-at-risk.

The axiomatic view goes back to Artzner, Delbaen, Eber and Heath (1999); the treatment of distributions with atoms, where several plausible definitions disagree, is due to Acerbi and Tasche (2002) and Rockafellar and Uryasev (2002). This mission follows Section 2.2.3 of Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007, doi:10.1142/6478), pp. 48–58, together with Proposition 2.74 on p. 109.

Setting

All outcomes are profit variables: larger values are better. Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space and YYY an integrable real random variable with distribution function G(u)=P{Y≤u}G(u)=\mathbb P\{Y\le u\}G(u)=P{Y≤u} and left-continuous quantile function

G−1(p)=inf⁡{u:G(u)≥p},0<p≤1.G^{-1}(p)=\inf\{u : G(u)\ge p\},\qquad 0<p\le1 .G−1(p)=inf{u:G(u)≥p},0<p≤1.

For 0<α≤10<\alpha\le10<α≤1 the average value-at-risk is the lower-tail average

AV@Rα(Y)=1α∫0αG−1(u) du,\mathbb{AV@R}_\alpha(Y)=\frac1\alpha\int_0^\alpha G^{-1}(u)\,du ,AV@Rα​(Y)=α1​∫0α​G−1(u)du,

so that AV@R1(Y)=EY\mathbb{AV@R}_1(Y)=\mathbb EYAV@R1​(Y)=EY, and the average value-at-risk deviation is AV@RDα(Y)=EY−AV@Rα(Y)\mathbb{AV@R}\mathbb D_\alpha(Y)=\mathbb EY-\mathbb{AV@R}_\alpha(Y)AV@RDα​(Y)=EY−AV@Rα​(Y). When GGG jumps at G−1(α)G^{-1}(\alpha)G−1(α), the two levels

αG+=inf⁡{G(u):G(u)≥α},αG−=sup⁡{G(u):G(u)<α}\alpha^+_G=\inf\{G(u):G(u)\ge\alpha\},\qquad \alpha^-_G=\sup\{G(u):G(u)<\alpha\}αG+​=inf{G(u):G(u)≥α},αG−​=sup{G(u):G(u)<α}

satisfy αG−≤α≤αG+\alpha^-_G\le\alpha\le\alpha^+_GαG−​≤α≤αG+​. Write [y]−=−min⁡(y,0)[y]^-=-\min(y,0)[y]−=−min(y,0) and [y]+=max⁡(y,0)[y]^+=\max(y,0)[y]+=max(y,0). Second-order stochastic dominance Y(1)≺SSDY(2)Y^{(1)}\prec_{SSD}Y^{(2)}Y(1)≺SSD​Y(2) means E U(Y(1))≤E U(Y(2))\mathbb E\,U(Y^{(1)})\le\mathbb E\,U(Y^{(2)})EU(Y(1))≤EU(Y(2)) for every nondecreasing concave UUU for which both expectations exist; Y(1)Y^{(1)}Y(1), Y(2)Y^{(2)}Y(2) are comonotone if P{Y(1)≤u,Y(2)≤v}=min⁡(G1(u),G2(v))\mathbb P\{Y^{(1)}\le u, Y^{(2)}\le v\}=\min(G_1(u),G_2(v))P{Y(1)≤u,Y(2)≤v}=min(G1​(u),G2​(v)) for all u,vu,vu,v.

In the Lean development, in the namespace RiskFunctionals.AVaR, these objects are distributionFunction, quantileFunction (both of the law P.map Y), averageValueAtRisk P Y α, avarDeviation P Y α, alphaPlus, alphaMinus, SSD and Comonotone.

Formalization targets

Goal: Theorem 2.34

For integrable YYY and 0<α≤10<\alpha\le10<α≤1:

  1. AV@Rα(Y)=max⁡{x−1αE([Y−x]−):x∈R}\displaystyle\mathbb{AV@R}_\alpha(Y)=\max\Big\{x-\frac1\alpha\mathbb E([Y-x]^-) : x\in\mathbb R\Big\}AV@Rα​(Y)=max{x−α1​E([Y−x]−):x∈R}, the maximum attained;
  2. AV@Rα(Y)=min⁡{E(YZ):EZ=1, 0≤Z≤1α}\displaystyle\mathbb{AV@R}_\alpha(Y)=\min\Big\{\mathbb E(YZ) : \mathbb EZ=1,\ 0\le Z\le\frac1\alpha\Big\}AV@Rα​(Y)=min{E(YZ):EZ=1, 0≤Z≤α1​}, the minimum attained;

and, if G−1(α)G^{-1}(\alpha)G−1(α) is finite,

  1. AV@Rα(Y)=G−1(α)−1αE([Y−G−1(α)]−)=G−1(α)−1α∫−∞G−1(α)(G−1(α)−u) dG(u)\displaystyle\mathbb{AV@R}_\alpha(Y)=G^{-1}(\alpha)-\frac1\alpha\mathbb E([Y-G^{-1}(\alpha)]^-)=G^{-1}(\alpha)-\frac1\alpha\int_{-\infty}^{G^{-1}(\alpha)}(G^{-1}(\alpha)-u)\,dG(u)AV@Rα​(Y)=G−1(α)−α1​E([Y−G−1(α)]−)=G−1(α)−α1​∫−∞G−1(α)​(G−1(α)−u)dG(u);
  2. AV@Rα(Y)=αG−αE[Y∣Y<G−1(α)]+α−αG−αG−1(α)\displaystyle\mathbb{AV@R}_\alpha(Y)=\frac{\alpha^-_G}{\alpha}\mathbb E[Y\mid Y<G^{-1}(\alpha)]+\frac{\alpha-\alpha^-_G}{\alpha}G^{-1}(\alpha)AV@Rα​(Y)=ααG−​​E[Y∣Y<G−1(α)]+αα−αG−​​G−1(α);
  3. AV@Rα(Y)=αG+αE[Y∣Y≤G−1(α)]−αG+−ααG−1(α)\displaystyle\mathbb{AV@R}_\alpha(Y)=\frac{\alpha^+_G}{\alpha}\mathbb E[Y\mid Y\le G^{-1}(\alpha)]-\frac{\alpha^+_G-\alpha}{\alpha}G^{-1}(\alpha)AV@Rα​(Y)=ααG+​​E[Y∣Y≤G−1(α)]−ααG+​−α​G−1(α).

The goal is the conjunction of the five parts, stated as printed. G−1(α)G^{-1}(\alpha)G−1(α) is finite for every α<1\alpha<1α<1, and for α=1\alpha=1α=1 exactly when YYY is essentially bounded above; parts 3–5 presuppose it. At α=1\alpha=1α=1 with YYY not essentially bounded above, the attainment claim of part 1 is false (see Beyond the paper), so the goal as printed is expected to be disprovable there.

Milestones

  • p. 49 and (2.18): αG+=G(G−1(α))\alpha^+_G=G(G^{-1}(\alpha))αG+​=G(G−1(α)), αG−=G(G−1(α)−)\alpha^-_G=G(G^{-1}(\alpha)-)αG−​=G(G−1(α)−), αG−≤α≤αG+\alpha^-_G\le\alpha\le\alpha^+_GαG−​≤α≤αG+​, P{Y≤G−1(α)}=αG+\mathbb P\{Y\le G^{-1}(\alpha)\}=\alpha^+_GP{Y≤G−1(α)}=αG+​, P{Y<G−1(α)}=αG−\mathbb P\{Y<G^{-1}(\alpha)\}=\alpha^-_GP{Y<G−1(α)}=αG−​.
  • (2.24): G−1(α)G^{-1}(\alpha)G−1(α) maximizes x↦x−1αE([Y−x]−)x\mapsto x-\frac1\alpha\mathbb E([Y-x]^-)x↦x−α1​E([Y−x]−).
  • (2.17): EY=α AV@Rα(Y)−(1−α) AV@R1−α(−Y)\mathbb EY=\alpha\,\mathbb{AV@R}_\alpha(Y)-(1-\alpha)\,\mathbb{AV@R}_{1-\alpha}(-Y)EY=αAV@Rα​(Y)−(1−α)AV@R1−α​(−Y) for 0<α<10<\alpha<10<α<1.
  • Proposition 2.35 (i)–(vii): translation equivariance, concavity, isotonicity with respect to ≺SSD\prec_{SSD}≺SSD​ and AV@Rα(Y)≤AV@Rα(E(Y∣F1))\mathbb{AV@R}_\alpha(Y)\le\mathbb{AV@R}_\alpha(\mathbb E(Y\mid\mathcal F_1))AV@Rα​(Y)≤AV@Rα​(E(Y∣F1​)), positive homogeneity, AV@RDα≥0\mathbb{AV@R}\mathbb D_\alpha\ge0AV@RDα​≥0, Lipschitz continuity on L1L_1L1​, comonotone additivity.
  • Proposition 2.36: Y(1)≺SSDY(2)Y^{(1)}\prec_{SSD}Y^{(2)}Y(1)≺SSD​Y(2) iff AV@Rα(Y(1))≤AV@Rα(Y(2))\mathbb{AV@R}_\alpha(Y^{(1)})\le\mathbb{AV@R}_\alpha(Y^{(2)})AV@Rα​(Y(1))≤AV@Rα​(Y(2)) for all 0<α≤10<\alpha\le10<α≤1.
  • Proposition 2.37: for nonconstant integrable YYY, α↦AV@Rα(Y)\alpha\mapsto\mathbb{AV@R}_\alpha(Y)α↦AV@Rα​(Y) is continuous and nondecreasing on (0,1](0,1](0,1] and tends to ess inf⁡Y\operatorname{ess\,inf}YessinfY as α↓0\alpha\downarrow0α↓0.
  • Example 2.40 (newsboy problem): with purchase price bbb, selling price s>bs>bs>b and refund r<br<br<b, the maximal expected profit is (s−b) AV@Rα(Y)(s-b)\,\mathbb{AV@R}_\alpha(Y)(s−b)AV@Rα​(Y) with α=s−bs−r\alpha=\frac{s-b}{s-r}α=s−rs−b​, attained at the order size G−1(α)G^{-1}(\alpha)G−1(α).
  • Proposition 2.74: min⁡a{E([Y−a]+)+1−ααE([Y−a]−)}=AV@RDα(Y)\min_a\{\mathbb E([Y-a]^+)+\frac{1-\alpha}{\alpha}\mathbb E([Y-a]^-)\}=\mathbb{AV@R}\mathbb D_\alpha(Y)mina​{E([Y−a]+)+α1−α​E([Y−a]−)}=AV@RDα​(Y), the minimum attained, for 0<α≤10<\alpha\le10<α≤1 as printed.

Beyond the paper

A strengthened variant of Proposition 2.37 drops the hypothesis that YYY is nonconstant: for Y≡cY\equiv cY≡c every average value-at-risk equals c=ess inf⁡Yc=\operatorname{ess\,inf}Yc=essinfY, and the book's argument never uses the hypothesis.

Two corrected variants address the endpoint α=1\alpha=1α=1. For YYY integrable but not essentially bounded above (for instance exponential), x−E([Y−x]−)=Emin⁡(Y,x)<EY=AV@R1(Y)x-\mathbb E([Y-x]^-)=\mathbb E\min(Y,x)<\mathbb EY=\mathbb{AV@R}_1(Y)x−E([Y−x]−)=Emin(Y,x)<EY=AV@R1​(Y) for every xxx, so the maximum in (2.19) is not attained; likewise E([Y−a]+)>0=AV@RD1(Y)\mathbb E([Y-a]^+)>0=\mathbb{AV@R}\mathbb D_1(Y)E([Y−a]+)>0=AV@RD1​(Y) for every aaa, so the minimum in (2.112) is not attained. The corrected Theorem 2.34 asserts part 1 only when G−1(α)G^{-1}(\alpha)G−1(α) is finite, and the corrected Proposition 2.74 adds the same hypothesis; both leave everything else unchanged.

Significance

Theorem 2.34 is the toolkit through which the average value-at-risk is used. Representation 1 makes it the optimal value of a one-dimensional concave maximization, which is how it enters stochastic programs and the newsboy-type models of Examples 2.39–2.40. Representation 2 exhibits it as an infimum of linear functionals over an explicit dual set, which yields concavity, L1L_1L1​-Lipschitz continuity and the link to the general dual representation of acceptability functionals. Representations 3–5 are the computational formulas for discrete distributions, where the naive "average of the outcomes below the quantile" is wrong. Proposition 2.36 shows that the family (AV@Rα)α(\mathbb{AV@R}_\alpha)_\alpha(AV@Rα​)α​ characterizes second-order dominance, and Proposition 2.74 identifies the deviation as a minimal-loss functional.

The results are classical and proved in the literature. What the mission adds is a machine-checked version in the book's conventions: profit variables, the lower tail, the left-continuous quantile, the dual set in L∞L_\inftyL∞​ with bound 1/α1/\alpha1/α, and general distributions with atoms. The platform holds related results in other conventions: the Rockafellar–Uryasev minimization formula for loss functions and upper tails, an open loss-side dual representation on L∞L_\inftyL∞​, and expected-shortfall properties on finite state spaces; none states these representations for profit variables on a general probability space.

Difficulty

Everything happens where GGG has an atom at G−1(α)G^{-1}(\alpha)G−1(α). A proof that pretends GGG is continuous, so that P{Y≤G−1(α)}=α\mathbb P\{Y\le G^{-1}(\alpha)\}=\alphaP{Y≤G−1(α)}=α, covers none of the cases the theorem was written for: the optimal dual variable must put a fractional weight on the event {Y=G−1(α)}\{Y=G^{-1}(\alpha)\}{Y=G−1(α)}, and representations 4 and 5 differ from each other precisely by the jump. Passing between integrals over Ω\OmegaΩ, integrals against the law, and Lebesgue integrals of the quantile function over (0,α](0,\alpha](0,α] needs the quantile transform for arbitrary distributions. The endpoint α=1\alpha=1α=1 is genuinely different: there G−1(1)G^{-1}(1)G−1(1) may be infinite and the maximum in (2.19) and the minimum in (2.112) are then not attained: the book's statements fail there, and the corrected variants carry the finiteness condition.

Formalization scope

A random variable is a measurable, integrable Y:Ω→RY:\Omega\to\mathbb RY:Ω→R on a probability space; AV@Rα(Y)\mathbb{AV@R}_\alpha(Y)AV@Rα​(Y) is computed from the law of YYY and so depends only on its distribution. The quantile function is real-valued; wherever it is evaluated at a point α\alphaα, the statement assumes G(u)≥αG(u)\ge\alphaG(u)≥α for some uuu. Maxima and minima are stated as attained greatest and least elements of the value sets, never as bare suprema or infima. In the dual representation ZZZ ranges over measurable functions with ∫Z dP=1\int Z\,d\mathbb P=1∫ZdP=1 and 0≤Z≤1/α0\le Z\le1/\alpha0≤Z≤1/α almost surely. Conditional expectations given an event are integrals against the conditional probability measure; when the event is null its coefficient αG±\alpha^\pm_GαG±​ is 000 as well. The limit at α↓0\alpha\downarrow0α↓0 is taken in the extended reals, since ess inf⁡Y\operatorname{ess\,inf}YessinfY may be −∞-\infty−∞.

A trivializing formalization is ruled out: writing (2.19) or (2.20) with sSup/sInf and no attainment, or using an upper-tail, loss-side conditional value-at-risk in place of the book's lower-tail functional, would change or empty the statement; neither is done.

Contributions welcome: the quantile transform for general laws, the change of variables between Ω\OmegaΩ, the law and (0,1)(0,1)(0,1), and the Rockafellar–Uryasev argument are reusable across the rest of this series (Kusuoka and distortion representations, nested average value-at-risk).

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. https://doi.org/10.1142/6478
  • R. T. Rockafellar, S. Uryasev, Optimization of conditional value-at-risk, Journal of Risk 2(3), 2000. https://doi.org/10.21314/JOR.2000.038
  • R. T. Rockafellar, S. Uryasev, Conditional value-at-risk for general loss distributions, Journal of Banking & Finance 26(7), 2002. https://doi.org/10.1016/S0378-4266(02)00271-6
  • C. Acerbi, D. Tasche, On the coherence of expected shortfall, Journal of Banking & Finance 26(7), 2002. https://doi.org/10.1016/S0378-4266(02)00283-2
  • P. Artzner, F. Delbaen, J.-M. Eber, D. Heath, Coherent measures of risk, Mathematical Finance 9(3), 1999. https://doi.org/10.1111/1467-9965.00068
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Functional AnalysisOperations ResearchOptimization+1·Captain: Shuze Chen

Modeling, Measuring and Managing Risk IV: Kusuoka Representations of Version-Independent Acceptability FunctionalsTextbook

Motivation

Risk measures used in portfolio optimization, insurance pricing and regulation are almost always law invariant: they assign a number to a random profit YYY that depends only on its distribution, not on the scenario in which each outcome occurs. Kusuoka (Kusuoka 2001) showed that on a non-atomic space every law-invariant coherent risk measure is the worst case, over a family of weightings, of mixtures of one elementary functional, the average value-at-risk (also called conditional value-at-risk or expected shortfall). This reduces the design and the computation of law-invariant risk measures to the choice of a set of probability measures on the interval of confidence levels, and it underlies the use of the average value-at-risk as the building block of spectral and distortion risk measures.

This mission formalizes the version of Kusuoka's theorem proved in G. Ch. Pflug and W. Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007, §2.2.4, Theorem 2.45), stated for acceptability functionals of profit variables on LpL_pLp​, 1≤p<∞1\le p<\infty1≤p<∞, together with the coupling and realization results its proof uses and a worked example from the same section.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space. It is non-atomic if no measurable set AAA with P(A)>0\mathbb P(A)>0P(A)>0 has only subsets of probability 000 or P(A)\mathbb P(A)P(A). Fix 1≤p<∞1\le p<\infty1≤p<∞ and the conjugate exponent qqq, 1/p+1/q=11/p+1/q=11/p+1/q=1; LpL_pLp​ is the space of real random variables with finite ppp-th moment (identified when equal almost surely) and LqL_qLq​ its dual, paired by E(YZ)\mathbb E(YZ)E(YZ).

For YYY with distribution function G(u)=P{Y≤u}G(u)=\mathbb P\{Y\le u\}G(u)=P{Y≤u}, the quantile function is G−1(p)=inf⁡{u:G(u)≥p}G^{-1}(p)=\inf\{u: G(u)\ge p\}G−1(p)=inf{u:G(u)≥p}, 0<p≤10<p\le10<p≤1, and the average value-at-risk at level 0<α≤10<\alpha\le10<α≤1 is the lower-tail average

AV@Rα(Y)=1α∫0αG−1(u) du.\mathbb{AV@R}_\alpha(Y)=\frac1\alpha\int_0^\alpha G^{-1}(u)\,du .AV@Rα​(Y)=α1​∫0α​G−1(u)du.

The book uses profit variables, so larger values are better and AV@Rα\mathbb{AV@R}_\alphaAV@Rα​ averages the worst α\alphaα-fraction of outcomes; AV@R1(Y)=EY\mathbb{AV@R}_1(Y)=\mathbb EYAV@R1​(Y)=EY.

A real valued A:Lp→R\mathcal A:L_p\to\mathbb RA:Lp​→R is an acceptability functional if it is translation equivariant, A(Y+c)=A(Y)+c\mathcal A(Y+c)=\mathcal A(Y)+cA(Y+c)=A(Y)+c (A1), concave (A2), and monotone, Y(1)≤Y(2)Y^{(1)}\le Y^{(2)}Y(1)≤Y(2) a.s. ⇒A(Y(1))≤A(Y(2))\Rightarrow\mathcal A(Y^{(1)})\le\mathcal A(Y^{(2)})⇒A(Y(1))≤A(Y(2)) (A3). It is version-independent if A(Y(1))=A(Y(2))\mathcal A(Y^{(1)})=\mathcal A(Y^{(2)})A(Y(1))=A(Y(2)) whenever Y(1)Y^{(1)}Y(1) and Y(2)Y^{(2)}Y(2) have the same distribution. A dual representation is

A(Y)=inf⁡{E(YZ)−A(Z):Z∈ZA},ZA⊆Lq,\mathcal A(Y)=\inf\{\mathbb E(YZ)-A(Z): Z\in\mathcal Z_{\mathcal A}\},\qquad \mathcal Z_{\mathcal A}\subseteq L_q,A(Y)=inf{E(YZ)−A(Z):Z∈ZA​},ZA​⊆Lq​,

and (A,ZA)(A,\mathcal Z_{\mathcal A})(A,ZA​) is version-independent if equally distributed Z,Z~Z,\tilde ZZ,Z~ are both or neither in ZA\mathcal Z_{\mathcal A}ZA​, with A(Z)=A(Z~)A(Z)=A(\tilde Z)A(Z)=A(Z~). Theorem 2.45 adds the conditions (C1) A=0A=0A=0, (C2) every Z∈ZAZ\in\mathcal Z_{\mathcal A}Z∈ZA​ is non-negative, (C3) every Z∈ZAZ\in\mathcal Z_{\mathcal A}Z∈ZA​ has EZ=1\mathbb E Z=1EZ=1.

Formalization targets

Goal: Theorem 2.45(i)

Under (C1), (C2) and (C3) there is a family G\mathcal GG of probability measures on (0,1](0,1](0,1], fixed independently of YYY, such that for every Y∈LpY\in L_pY∈Lp​

A(Y)=inf⁡{∫(0,1]AV@Rα(Y) dm(α):m∈G}.(2.37)\mathcal A(Y)=\inf\Big\{\int_{(0,1]}\mathbb{AV@R}_\alpha(Y)\,dm(\alpha): m\in\mathcal G\Big\}. \tag{2.37}A(Y)=inf{∫(0,1]​AV@Rα​(Y)dm(α):m∈G}.(2.37)

Milestones

  • Theorem A.2 (p. 266): on a non-atomic probability space every probability law on a complete separable metric space is the law of some random variable.
  • Proposition 1.8 (p. 11): for given marginals, the covariance is maximal under the comonotone coupling and minimal under the antimonotone coupling.
  • Eq. (2.38) (p. 61): under (C1), A(Y)=inf⁡{∫01F−1(u)G−1(1−u) du:G∈G}\mathcal A(Y)=\inf\{\int_0^1F^{-1}(u)G^{-1}(1-u)\,du: G\in\mathcal G\}A(Y)=inf{∫01​F−1(u)G−1(1−u)du:G∈G}, with FFF the law of YYY and G\mathcal GG the laws of the Z∈ZAZ\in\mathcal Z_{\mathcal A}Z∈ZA​.
  • Theorem 2.45(ii)–(iv) (p. 60): the representations with non-negative measures under (C1)+(C2), with two families of measures under (C1),
A(Y)=inf⁡{∫AV@Rα(Y) dmG(1)(α)−∫AV@R1−α(−Y) dmG(2)(α)},\mathcal A(Y)=\inf\Big\{\int\mathbb{AV@R}_\alpha(Y)\,dm^{(1)}_G(\alpha)-\int\mathbb{AV@R}_{1-\alpha}(-Y)\,dm^{(2)}_G(\alpha)\Big\},A(Y)=inf{∫AV@Rα​(Y)dmG(1)​(α)−∫AV@R1−α​(−Y)dmG(2)​(α)},

and in general with an additional penalty −A~{G}-\tilde A\{G\}−A~{G} and AV@Rα(−Y)\mathbb{AV@R}_\alpha(-Y)AV@Rα​(−Y) in the second integral.

  • Example 2.46, Eq. (2.41) (p. 64): E(Y)−12E∣Y−EY∣=inf⁡{∫(0,1]AV@Rα(Y) dm(α):m∈P(0,1], ∫(0,1)v−1 dm(v)≤1}\mathbb E(Y)-\tfrac12\mathbb E|Y-\mathbb EY|=\inf\{\int_{(0,1]}\mathbb{AV@R}_\alpha(Y)\,dm(\alpha): m\in\mathcal P(0,1],\ \int_{(0,1)}v^{-1}\,dm(v)\le1\}E(Y)−21​E∣Y−EY∣=inf{∫(0,1]​AV@Rα​(Y)dm(α):m∈P(0,1], ∫(0,1)​v−1dm(v)≤1}.

Significance

The result. The Kusuoka representation says that the average values-at-risk are the extreme points of law-invariant acceptability: any such functional is determined by a set of mixing measures on the confidence levels. Consequences used in the rest of the book and in the literature include the identification of comonotone additive functionals with single mixtures (Choquet representations), explicit representations of mean–deviation functionals such as (2.41), and the reduction of optimization problems with law-invariant risk constraints to families of average value-at-risk constraints. The statement for LpL_pLp​, rather than for bounded variables, is what makes it applicable to models with unbounded returns.

Formalizing it. The theorem is proved in the book and in the literature; it has not been machine-checked. Formalizing it requires infrastructure that is reusable beyond this mission: the quantile function and the average value-at-risk on LpL_pLp​, the realization of a prescribed joint law on an arbitrary non-atomic probability space, and the Hardy–Littlewood-type rearrangement inequality behind the antimonotone coupling. Related platform results are in other conventions: a distortion functional of losses on L∞L_\inftyL∞​ as a single mixture of average values-at-risk (MultistageStochastic.distortion_avar_mixture, proved) and Schmeidler's comonotonic characterization on finite uniform spaces (RiskUncSets.Distortion.theorem_4_1, open). Neither covers the infimum over a family, profit variables, or LpL_pLp​.

Difficulty

The obvious argument is to write each Z∈ZAZ\in\mathcal Z_{\mathcal A}Z∈ZA​ as a mixing measure directly. This fails because E(YZ)\mathbb E(YZ)E(YZ) depends on the joint law of (Y,Z)(Y,Z)(Y,Z), not on the two marginals; the infimum must first be reduced to antimonotone couplings, which requires (a) that every coupling of the two marginals can be realized on the given space without leaving ZA\mathcal Z_{\mathcal A}ZA​, using version-independence of both A\mathcal AA and (A,ZA)(A,\mathcal Z_{\mathcal A})(A,ZA​) and non-atomicity, and (b) the extremal property of the antimonotone coupling for products of an LpL_pLp​ and an LqL_qLq​ variable, where quantile functions may be unbounded at both ends. The passage from G−1(1−u)G^{-1}(1-u)G−1(1−u) to a mixing measure is a Stieltjes integration by parts on (0,1)(0,1)(0,1) that must handle a point mass at 111, and the integrability of α↦AV@Rα(Y)\alpha\mapsto\mathbb{AV@R}_\alpha(Y)α↦AV@Rα​(Y), which tends to the essential infimum of YYY (possibly −∞-\infty−∞) as α→0\alpha\to0α→0. Non-atomicity cannot be dropped: the book's Counterexample on p. 63 is a version-independent functional on a two-point space without representation (2.37).

Formalization scope

Probability spaces are (Ω, ℱ, P) with IsProbabilityMeasure P; non-atomicity is the book's notion (no atoms), which is stronger than Mathlib's NoAtoms. Random variables are elements of Lp ℝ p P with 1 ≤ p, p ≠ ⊤, and dual variables elements of Lp ℝ q P with p.HolderConjugate q. The quantile function is the left-continuous inverse of the book's (1.3), evaluated only on (0,1)(0,1)(0,1) or inside integrals over (0,α](0,\alpha](0,α]; AV@Rα\mathbb{AV@R}_\alphaAV@Rα​ is the lower-tail average (2.15), not the upper-tail loss CVaR. Version-independence is "equal laws give equal values" (IdentDistrib). Every infimum is stated as a greatest lower bound in R\mathbb RR (IsGLB), which forces the indexing set to be nonempty and bounded below; measures on (0,1](0,1](0,1] are measures on R\mathbb RR with no mass outside (0,1](0,1](0,1]. The family G\mathcal GG is quantified before YYY: a family allowed to depend on YYY would reduce (2.37) to matching the single number A(Y)\mathcal A(Y)A(Y) by some mixture, a much weaker statement, and that reading is excluded. Each representation also asserts that every integrand is integrable against every measure of the family, so that no integral can take Lean's default value 000.

Beyond the paper. Two variant items accompany the goal. kusuoka_representation_strong ([Strengthened]) drops (C2) and (C3): for a real valued acceptability functional they follow from (A1), (A3) and the dual representation, since E(YZ)≥A(Y)\mathbb E(YZ)\ge\mathcal A(Y)E(YZ)≥A(Y) for every YYY forces EZ=1\mathbb EZ=1EZ=1 (constants) and Z≥0Z\ge0Z≥0 (scaled indicators). kusuoka_representation_probe ([Sharpness probe]) drops non-atomicity; it is expected to be false by the p. 63 Counterexample, and a disproof is the sought outcome. The printed proof of Theorem 2.45(iii) has a sign gap (it derives +∫AV@R1−α(−Y) dm(2)+\int\mathbb{AV@R}_{1-\alpha}(-Y)\,dm^{(2)}+∫AV@R1−α​(−Y)dm(2)); the statements (iii) and (iv) are kept as printed.

Contributions welcome: the quantile transform and realization of joint laws on non-atomic spaces, the rearrangement inequality on Lp×LqL_p\times L_qLp​×Lq​, and the integration-by-parts construction of the mixing measure, each of which can be submitted as a separate lemma.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007, §2.2.4 and Appendix A. https://doi.org/10.1142/6478
  • S. Kusuoka, On law invariant coherent risk measures, Advances in Mathematical Economics 3, 83–95, 2001. https://doi.org/10.1007/978-4-431-67891-5_4
  • W. Hoeffding, Masstabinvariante Korrelationstheorie, Schriften des Mathematischen Instituts der Universität Berlin 5, 179–233, 1940.
  • S. T. Rachev, Probability Metrics and the Stability of Stochastic Models, Wiley, 1991 (Lemma 2.5.1, cited for Theorem A.2).
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Functional AnalysisOperations ResearchOptimization+1·Captain: Shuze Chen

Modeling, Measuring and Managing Risk V: Dual Representation of Conditional Acceptability MappingsTextbook

Motivation

A risk measure that returns a single number answers the question "how acceptable is this random profit, seen from today?". Multi-period decision problems — portfolio rebalancing, insurance reserves, stochastic programs on scenario trees — need the same question asked at every later date, given the information available then. The answer is no longer a number but a random variable measurable with respect to the information available at that date. Section 2.3 of Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific, 2007, doi:10.1142/6478), sets up these conditional acceptability mappings axiomatically and gives them a dual representation modelled on the defining relation of the conditional expectation. The conditional average value-at-risk defined there is the building block of the nested risk measures used in multi-stage stochastic optimization (Chapter 3 of the same book), and of the time-consistent risk measures of Ruszczyński and Shapiro (doi:10.1287/moor.1060.0204) and Detlefsen and Scandolo (doi:10.1007/s00780-005-0159-6).

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space and F1⊆F\mathcal F_1\subseteq\mathcal FF1​⊆F a sub-σ\sigmaσ-field, the observable information. Fix p∈[1,∞)p\in[1,\infty)p∈[1,∞) and let qqq be its conjugate exponent, 1/p+1/q=11/p+1/q=11/p+1/q=1. Put Y=Lp(Ω,F,P)\mathcal Y=L_p(\Omega,\mathcal F,\mathbb P)Y=Lp​(Ω,F,P) and Y1=Lp(Ω,F1,P)\mathcal Y_1=L_p(\Omega,\mathcal F_1,\mathbb P)Y1​=Lp​(Ω,F1​,P), the subspace of classes with an F1\mathcal F_1F1​-measurable version. Random variables equal almost surely are identified, and every (in)equality between them holds almost surely. Variables are profits: larger is better.

A map A:Y→Y1\mathcal A:\mathcal Y\to\mathcal Y_1A:Y→Y1​ is a conditional acceptability mapping if for all Y,Y~∈YY,\tilde Y\in\mathcal YY,Y~∈Y

  • (CA1) A(Y+Y(1))=A(Y)+Y(1)\mathcal A(Y+Y^{(1)})=\mathcal A(Y)+Y^{(1)}A(Y+Y(1))=A(Y)+Y(1) for every Y(1)∈Y1Y^{(1)}\in\mathcal Y_1Y(1)∈Y1​;
  • (CA2) A(λY+(1−λ)Y~)≥λA(Y)+(1−λ)A(Y~)\mathcal A(\lambda Y+(1-\lambda)\tilde Y)\ge\lambda\mathcal A(Y)+(1-\lambda)\mathcal A(\tilde Y)A(λY+(1−λ)Y~)≥λA(Y)+(1−λ)A(Y~) for λ∈[0,1]\lambda\in[0,1]λ∈[0,1];
  • (CA3) Y≤Y~Y\le\tilde YY≤Y~ implies A(Y)≤A(Y~)\mathcal A(Y)\le\mathcal A(\tilde Y)A(Y)≤A(Y~).

It is positively homogeneous if A(λY)=λA(Y)\mathcal A(\lambda Y)=\lambda\mathcal A(Y)A(λY)=λA(Y) for λ>0\lambda>0λ>0, and upper semicontinuous if, for every B∈F1B\in\mathcal F_1B∈F1​, the real functional Y↦E(A(Y)1B)Y\mapsto\mathbb E(\mathcal A(Y)\mathbb 1_B)Y↦E(A(Y)1B​) is upper semicontinuous on Y\mathcal YY. For B∈F1B\in\mathcal F_1B∈F1​ and Z∈Lq(F)Z\in L_q(\mathcal F)Z∈Lq​(F) the dual function is

AB(Z)=inf⁡{E(YZ)−E(A(Y)1B):Y∈Y}∈[−∞,∞).A_B(Z)=\inf\{\mathbb E(YZ)-\mathbb E(\mathcal A(Y)\mathbb 1_B):Y\in\mathcal Y\}\in[-\infty,\infty).AB​(Z)=inf{E(YZ)−E(A(Y)1B​):Y∈Y}∈[−∞,∞).

For 0<α≤10<\alpha\le10<α≤1 and Y∈L1(F)Y\in L_1(\mathcal F)Y∈L1​(F), the conditional average value-at-risk AV@Rα(Y∣F1)\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)AV@Rα​(Y∣F1​) is a class in L1(F1)L_1(\mathcal F_1)L1​(F1​) such that, for every B∈F1B\in\mathcal F_1B∈F1​,

E(AV@Rα(Y∣F1)1B)=inf⁡{E(YZ):0≤Z≤1α1B, E(Z∣F1)=1B}.\mathbb E(\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)\mathbb 1_B)=\inf\Big\{\mathbb E(YZ):0\le Z\le\tfrac1\alpha\mathbb 1_B,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\Big\}.E(AV@Rα​(Y∣F1​)1B​)=inf{E(YZ):0≤Z≤α1​1B​, E(Z∣F1​)=1B​}.

When F1\mathcal F_1F1​ is trivial it reduces to the lower-tail average AV@Rα(Y)=1α∫0αG−1(u) du\mathbb{AV@R}_\alpha(Y)=\frac1\alpha\int_0^\alpha G^{-1}(u)\,duAV@Rα​(Y)=α1​∫0α​G−1(u)du of the left-continuous quantile function G−1(u)=inf⁡{v:G(v)≥u}G^{-1}(u)=\inf\{v:G(v)\ge u\}G−1(u)=inf{v:G(v)≥u} of YYY.

Formalization targets

Goal: Theorem 2.51

For an upper semicontinuous conditional acceptability mapping A\mathcal AA, every Y∈YY\in\mathcal YY∈Y and every B∈F1B\in\mathcal F_1B∈F1​,

E(A(Y)1B)=inf⁡Z∈Lq(F){E(YZ)−AB(Z):Z≥0, E(Z∣F1)=1B},\mathbb E(\mathcal A(Y)\mathbb 1_B)=\inf_{Z\in L_q(\mathcal F)}\{\mathbb E(YZ)-A_B(Z):Z\ge0,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\},E(A(Y)1B​)=Z∈Lq​(F)inf​{E(YZ)−AB​(Z):Z≥0, E(Z∣F1​)=1B​},

and if A\mathcal AA is positively homogeneous then ABA_BAB​ takes only the values 000 (on SB={Z:AB(Z)≥0}S_B=\{Z:A_B(Z)\ge0\}SB​={Z:AB​(Z)≥0}) and −∞-\infty−∞ (off SBS_BSB​), and

E(A(Y)1B)=inf⁡Z∈SB{E(YZ):Z≥0, E(Z∣F1)=1B}.\mathbb E(\mathcal A(Y)\mathbb 1_B)=\inf_{Z\in S_B}\{\mathbb E(YZ):Z\ge0,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\}.E(A(Y)1B​)=Z∈SB​inf​{E(YZ):Z≥0, E(Z∣F1​)=1B​}.

Milestones

  1. Eqs. (2.48)–(2.49): the unconstrained form, E(A(Y)1B)=inf⁡Z∈Lq{E(YZ)−AB(Z)}\mathbb E(\mathcal A(Y)\mathbb 1_B)=\inf_{Z\in L_q}\{\mathbb E(YZ)-A_B(Z)\}E(A(Y)1B​)=infZ∈Lq​​{E(YZ)−AB​(Z)}.
  2. Theorem 2.54: a conditional acceptability mapping that is bounded below, in the order of the cone K\mathcal KK of a.s. non-negative elements of Lp(F1)L_p(\mathcal F_1)Lp​(F1​), by a bounded set on a neighbourhood of one point is continuous.
  3. Proposition 2.57 (i)–(ix): version-independence and unique existence in L1(F1)L_1(\mathcal F_1)L1​(F1​), concavity with F1\mathcal F_1F1​-measurable weights, homogeneity under bounded non-negative F1\mathcal F_1F1​-measurable factors, monotonicity, AV@Rα(Y∣F1)=Y\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)=YAV@Rα​(Y∣F1​)=Y for F1\mathcal F_1F1​-measurable YYY, reduction to AV@Rα(Y)\mathbb{AV@R}_\alpha(Y)AV@Rα​(Y) for trivial F1\mathcal F_1F1​, monotonicity in α\alphaα, AV@R1(Y∣F1)=E(Y∣F1)\mathbb{AV@R}_1(Y\mid\mathcal F_1)=\mathbb E(Y\mid\mathcal F_1)AV@R1​(Y∣F1​)=E(Y∣F1​), and the tower inequalities (2.58).

Further items of the section, stated faithfully but not milestones:

  • Example 2.53(a): E(E(Y∣F1)1B)=inf⁡{E(YZ):0≤Z≤1, E(Z∣F1)=1B}=E(Y1B)\mathbb E(\mathbb E(Y\mid\mathcal F_1)\mathbb 1_B)=\inf\{\mathbb E(YZ):0\le Z\le1,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\}=\mathbb E(Y\mathbb 1_B)E(E(Y∣F1​)1B​)=inf{E(YZ):0≤Z≤1, E(Z∣F1​)=1B​}=E(Y1B​), and E(⋅∣F1)\mathbb E(\cdot\mid\mathcal F_1)E(⋅∣F1​) maps Lp(F)L_p(\mathcal F)Lp​(F) onto Lp(F1)L_p(\mathcal F_1)Lp​(F1​).
  • Theorem 2.52: a closed convex S⊆L∞(F)S\subseteq L_\infty(\mathcal F)S⊆L∞​(F) with 1∈S\mathbb 1\in S1∈S and Z1B∈SZ\mathbb 1_B\in SZ1B​∈S defines, through E(Y1∗1B)=inf⁡Z∈S{E(YZ):Z≥0, E(Z∣F1)=1B}\mathbb E(Y_1^*\mathbb 1_B)=\inf_{Z\in S}\{\mathbb E(YZ):Z\ge0,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\}E(Y1∗​1B​)=infZ∈S​{E(YZ):Z≥0, E(Z∣F1​)=1B​}, a positively homogeneous u.s.c. conditional acceptability mapping on L1L_1L1​.
  • Example 2.53(b): AV@Rα(⋅∣F1)\mathbb{AV@R}_\alpha(\cdot\mid\mathcal F_1)AV@Rα​(⋅∣F1​) is well defined on L1(F)L_1(\mathcal F)L1​(F) and is a positively homogeneous u.s.c. conditional acceptability mapping.

Significance

Theorem 2.51 says that a conditional acceptability mapping is determined by the family of real concave functionals Y↦E(A(Y)1B)Y\mapsto\mathbb E(\mathcal A(Y)\mathbb 1_B)Y↦E(A(Y)1B​), and that each of these is an infimum of expectations under densities whose conditional expectation is 1B\mathbb 1_B1B​. It turns the axioms (CA1)–(CA3) into a computable object: a dual set, one per observable event, which is what stochastic programs with conditional risk constraints actually optimize over. The converse direction (Theorem 2.52 and Example 2.53) is how the book manufactures conditional versions of the average value-at-risk and of other dual-representable functionals, and Proposition 2.57 lists the properties used later when these mappings are nested over a tree.

None of these results is formalized. Mathlib has conditional expectation, LpL_pLp​ spaces, Hölder duality and the Hahn–Banach separation theorem, but no Fenchel–Moreau theorem on LpL_pLp​ and no conditional risk mappings. Prove2Me poses, as an open problem, Ruszczyński and Shapiro's representation of lower semicontinuous conditional risk mappings (CondRiskMap.Repr.theorem_1); it is stated pointwise in ω\omegaω on abstract paired spaces with loss variables, not in the integrated form over events B∈F1B\in\mathcal F_1B∈F1​ used here. Two of the printed statements are false as stated, and the mission records this: see Beyond the paper below.

Difficulty

The obvious route to (2.45) applies the Fenchel–Moreau theorem to hBh_BhB​ and then shows that the dual function is −∞-\infty−∞ off the constraint set. The first step needs the biconjugation theorem for concave upper semicontinuous real functionals on LpL_pLp​, with the dual identified as LqL_qLq​, for every p∈[1,∞)p\in[1,\infty)p∈[1,∞) including p=1p=1p=1 where the dual is L∞L_\inftyL∞​; none of this is in Mathlib. The second step must handle the constraint E(Z∣F1)=1B\mathbb E(Z\mid\mathcal F_1)=\mathbb 1_BE(Z∣F1​)=1B​ as an equality of conditional expectations, not of expectations. For Theorem 2.52 the natural argument builds a measure on F1\mathcal F_1F1​ from the infimum and takes its Radon–Nikodym derivative; the additivity of that set function is exactly what fails for general SSS.

Formalization scope

Y\mathcal YY is Lp ℝ p P with 1 ≤ p, p ≠ ∞, and Y1\mathcal Y_1Y1​ is Mathlib's subspace lpMeas ℝ ℝ m p P of classes a.e. equal to an m-measurable function, where m ≤ mΩ is F1\mathcal F_1F1​; the dual exponent is given by p.HolderConjugate q. Pointwise axioms are almost sure. E(Z∣F1)\mathbb E(Z\mid\mathcal F_1)E(Z∣F1​) is Mathlib's P[Z|m]. Every infimum, and the dual function ABA_BAB​, is computed in EReal, so an empty constraint set gives +∞+\infty+∞, an unbounded one −∞-\infty−∞, and no infimum has a junk value; the difference E(YZ)−AB(Z)\mathbb E(YZ)-A_B(Z)E(YZ)−AB​(Z) always has a real first term. Upper semicontinuity is that of the real functionals indexed by B∈F1B\in\mathcal F_1B∈F1​, as the book defines it — reading it as upper semicontinuity of the map into Lp(F1)L_p(\mathcal F_1)Lp​(F1​), or replacing the infimum by an unconstrained one over all of LqL_qLq​, would change the theorem. The conditional AV@R\mathbb{AV@R}AV@R is a predicate on classes in L1(F1)L_1(\mathcal F_1)L1​(F1​), never a construction: its existence is a stated result, not an assumption. Profits, not losses: the lower tail is averaged. Version-independence (Definition 2.55, used in Proposition 2.57(i)) is stated pointwise: the conditional AV@Rα\mathbb{AV@R}_\alphaAV@Rα​ is almost surely one fixed function of the conditional distribution function G(⋅∣F1)(ω)G(\cdot\mid\mathcal F_1)(\omega)G(⋅∣F1​)(ω) of (2.56), for every YYY.

Needed infrastructure: the Fenchel–Moreau theorem on LpL_pLp​, the LpL_pLp​–LqL_qLq​ duality pairing, and Radon–Nikodym on a sub-σ\sigmaσ-field. All three are reusable well beyond this mission.

Beyond the paper. Two corrected variants are posed beside the faithful statements. Theorem 2.52, corrected (findings F1, F2) adds that SSS is bounded in L∞L_\inftyL∞​ and closed under pasting along F1\mathcal F_1F1​; without pasting, S={E(Z2)≤1, ∥Z∥∞≤2}S=\{\mathbb E(Z^2)\le1,\ \|Z\|_\infty\le2\}S={E(Z2)≤1, ∥Z∥∞​≤2} on [0,1][0,1][0,1] makes the right side of (2.50) non-additive in BBB, and without boundedness S=L∞S=L_\inftyS=L∞​ with Y(ω)=−ω−1/2Y(\omega)=-\omega^{-1/2}Y(ω)=−ω−1/2 makes it −∞-\infty−∞. Proposition 2.57, corrected (finding F3) replaces the second inequality of (2.58), E[AV@Rα(Y∣F2)∣F1]≤AV@Rα(E(Y∣F2)∣F1)\mathbb E[\mathbb{AV@R}_\alpha(Y\mid\mathcal F_2)\mid\mathcal F_1]\le\mathbb{AV@R}_\alpha(\mathbb E(Y\mid\mathcal F_2)\mid\mathcal F_1)E[AV@Rα​(Y∣F2​)∣F1​]≤AV@Rα​(E(Y∣F2​)∣F1​), which fails on two equally likely points with Y=(0,1)Y=(0,1)Y=(0,1), F1\mathcal F_1F1​ trivial, F2\mathcal F_2F2​ full and α=12\alpha=\frac12α=21​, by AV@Rα(Y∣F1)≤AV@Rα(E(Y∣F2)∣F1)\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)\le\mathbb{AV@R}_\alpha(\mathbb E(Y\mid\mathcal F_2)\mid\mathcal F_1)AV@Rα​(Y∣F1​)≤AV@Rα​(E(Y∣F2​)∣F1​). Disproofs of the faithful Theorem 2.52 and of the faithful Proposition 2.57 are welcome contributions, as are proofs of the variants.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. doi:10.1142/6478
  • A. Ruszczyński, A. Shapiro, Conditional risk mappings, Mathematics of Operations Research 31(3), 2006. doi:10.1287/moor.1060.0204
  • K. Detlefsen, G. Scandolo, Conditional and dynamic convex risk measures, Finance and Stochastics 9(4), 2005. doi:10.1007/s00780-005-0159-6
  • K. Nikodem, Continuity properties of convex-type set-valued maps, Journal of Inequalities in Pure and Applied Mathematics 4(3), Article 52, 2003. http://jipam.vu.edu.au
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Modeling, Measuring and Managing Risk II: Dual Representation of Acceptability FunctionalsTextbook

Motivation

Risk functionals assign a number to an uncertain profit and are used as objectives and constraints in portfolio selection, insurance and energy planning. Since the axiomatization of coherent risk measures by Artzner, Delbaen, Eber and Heath (Math. Finance 1999), the standard way to understand such a functional is through a dual representation: the functional is written as a worst case of expectations under a family of probability densities, penalized by a convex or concave function of the density. Föllmer and Schied (Finance Stoch. 2002) and Ruszczyński and Shapiro (Math. Oper. Res. 2006) established this representation for convex risk measures on L∞L_\inftyL∞​ and on paired spaces. Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007), develop the same theory on the profit side, for acceptability functionals (larger is better) and deviation risk functionals, on LpL_pLp​ spaces. Section 2.2 of their book recognizes these functionals by their dual representations. This mission formalizes that section and the conjugate duality of Appendix B it rests on.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a non-atomic probability space: no measurable AAA with P(A)>0P(A)>0P(A)>0 has every measurable subset of probability 000 or P(A)P(A)P(A) (the book assumes this throughout). Fix 1≤p<∞1\le p<\infty1≤p<∞ and q∈(1,∞]q\in(1,\infty]q∈(1,∞] with 1p+1q=1\frac1p+\frac1q=1p1​+q1​=1. Write Y=Lp(Ω,F,P)\mathcal Y=L_p(\Omega,\mathcal F,P)Y=Lp​(Ω,F,P) and Z=Lq(Ω,F,P)\mathcal Z=L_q(\Omega,\mathcal F,P)Z=Lq​(Ω,F,P), paired by

⟨Y,Z⟩=E(YZ)=∫ΩYZ dP.\langle Y,Z\rangle=\mathbb E(YZ)=\int_\Omega Y Z\,dP .⟨Y,Z⟩=E(YZ)=∫Ω​YZdP.

A functional is a map A:Y→[−∞,+∞]\mathcal A:\mathcal Y\to[-\infty,+\infty]A:Y→[−∞,+∞]; constants ccc are constant random variables. An acceptability functional satisfies

  • (A1) A(Y+c)=A(Y)+c\mathcal A(Y+c)=\mathcal A(Y)+cA(Y+c)=A(Y)+c,
  • (A2) A(λY(1)+(1−λ)Y(2))≥λA(Y(1))+(1−λ)A(Y(2))\mathcal A(\lambda Y^{(1)}+(1-\lambda)Y^{(2)})\ge\lambda\mathcal A(Y^{(1)})+(1-\lambda)\mathcal A(Y^{(2)})A(λY(1)+(1−λ)Y(2))≥λA(Y(1))+(1−λ)A(Y(2)) for 0≤λ≤10\le\lambda\le10≤λ≤1, and
  • (A3) Y(1)≤Y(2)Y^{(1)}\le Y^{(2)}Y(1)≤Y(2) a.s. ⇒A(Y(1))≤A(Y(2))\Rightarrow\mathcal A(Y^{(1)})\le\mathcal A(Y^{(2)})⇒A(Y(1))≤A(Y(2)).

Positive homogeneity (A4) is A(λY)=λA(Y)\mathcal A(\lambda Y)=\lambda\mathcal A(Y)A(λY)=λA(Y) for λ≥0\lambda\ge0λ≥0, and strictness (A5) is A(Y)≤E(Y)\mathcal A(Y)\le\mathbb E(Y)A(Y)≤E(Y). A deviation risk functional D\mathcal DD satisfies (D1) D(Y+c)=D(Y)\mathcal D(Y+c)=\mathcal D(Y)D(Y+c)=D(Y), (D2) convexity, and (D3) X≤Y⇒E(X)−D(X)≤E(Y)−D(Y)X\le Y\Rightarrow\mathbb E(X)-\mathcal D(X)\le\mathbb E(Y)-\mathcal D(Y)X≤Y⇒E(X)−D(X)≤E(Y)−D(Y). The acceptance set of A\mathcal AA is SA={Y:A(Y)≥0}\mathcal S_{\mathcal A}=\{Y:\mathcal A(Y)\ge0\}SA​={Y:A(Y)≥0}, and a set S\mathcal SS defines AS(Y)=sup⁡{a:Y−a∈S}\mathcal A_{\mathcal S}(Y)=\sup\{a: Y-a\in\mathcal S\}AS​(Y)=sup{a:Y−a∈S}.

The concave conjugate and the convex conjugate are

A+(Z)=inf⁡Y∈Y{E(YZ)−A(Y)},D∗(Z)=sup⁡Y∈Y{E(YZ)−D(Y)},\mathcal A^+(Z)=\inf_{Y\in\mathcal Y}\{\mathbb E(YZ)-\mathcal A(Y)\},\qquad \mathcal D^*(Z)=\sup_{Y\in\mathcal Y}\{\mathbb E(YZ)-\mathcal D(Y)\},A+(Z)=Y∈Yinf​{E(YZ)−A(Y)},D∗(Z)=Y∈Ysup​{E(YZ)−D(Y)},

and h∗∗(Y)=sup⁡Z{E(YZ)−h∗(Z)}h^{**}(Y)=\sup_{Z}\{\mathbb E(YZ)-h^*(Z)\}h∗∗(Y)=supZ​{E(YZ)−h∗(Z)}. A convex-type hhh is proper if h>−∞h>-\inftyh>−∞ everywhere and h<+∞h<+\inftyh<+∞ somewhere; a concave-type ggg is proper if −g-g−g is.

Formalization targets

Goal: Corollary 2.32, representation (2.11)

A proper upper semicontinuous acceptability functional satisfies, for every Y∈YY\in\mathcal YY∈Y,

A(Y)=inf⁡{E(YZ)−A+(Z): Z∈Lq, EZ=1, Z≥0},\mathcal A(Y)=\inf\{\mathbb E(YZ)-\mathcal A^+(Z):\ Z\in L_q,\ \mathbb EZ=1,\ Z\ge0\},A(Y)=inf{E(YZ)−A+(Z): Z∈Lq​, EZ=1, Z≥0},

and conversely, a functional represented in this form by any proper functional in place of A+\mathcal A^+A+ is upper semicontinuous and satisfies (A1)–(A3). Up to semicontinuity, acceptability functionals are exactly the penalized infima of expectations under probability densities.

Milestones

  1. Proposition 2.26: (A1) together with u.s.c., (A2), (A3), (A4) or (A5) make SA\mathcal S_{\mathcal A}SA​ closed, convex, monotone, a cone, or disjoint from {E<0}\{\mathbb E<0\}{E<0}, respectively.
  2. Proposition 2.27: the converse passage from a set S\mathcal SS to AS\mathcal A_{\mathcal S}AS​, as printed.
  3. Theorem B.1 (Fenchel–Moreau–Rockafellar): h∗∗=hh^{**}=hh∗∗=h for proper, l.s.c., convex hhh on LpL_pLp​.
  4. Theorem 2.30, (A)(i)–(iv) and (B)(vi)–(ix): sufficient conditions on a dual representation for (A1), (A4), version independence, (A3) and first-order dominance, and for (D1), (D4), version independence and (D3).
  5. Theorem 2.31: necessary conditions on the conjugate. Under (A1), A+(Z)>−∞\mathcal A^+(Z)>-\inftyA+(Z)>−∞ implies EZ=1\mathbb E Z=1EZ=1. Under (A4), A+∈{0,−∞}\mathcal A^+\in\{0,-\infty\}A+∈{0,−∞}. Under (A3), P{Z<0}>0P\{Z<0\}>0P{Z<0}>0 implies A+(Z)=−∞\mathcal A^+(Z)=-\inftyA+(Z)=−∞. Antitonicity under conditional expectation passes to A+\mathcal A^+A+. Items (v)–(vii) are the deviation mirrors.

Further items, not milestones: the first sentence of Theorem B.1 (h∗∗h^{**}h∗∗ is the largest l.s.c. convex minorant of a proper hhh) and the deviation half of Corollary 2.32, representation (2.12), each stated as printed.

Significance

The corollary is the profit-side, LpL_pLp​ form of the dual representation of convex risk measures. It turns a property of a functional into a constraint on its dual domain. Translation equivariance becomes the requirement that the densities ZZZ have mean one, and monotonicity becomes the requirement that they be nonnegative. This is how later chapters of the book compute with the average value-at-risk, distortion functionals and multi-period functionals: each is specified by its supergradient set. A machine-checked version gives these computations a common, verified foundation.

The results are classical and proved on paper; none is formalized in this form. The platform holds a loss-side analogue on abstract paired spaces with signed-measure duals (ConvexRiskFn.Dual.theorem_2_2) and a Fenchel–Moreau theorem in the same setting (ConvexRiskFn.Dual.theorem_2_1). Neither states the LpL_pLp​/LqL_qLq​, profit-side, density-constrained representation (2.11). Formalizing the chapter also checks its statements: three printed statements are false as written, and the mission poses a corrected form beside each faithful one.

Difficulty

Representation (2.11) needs the Fenchel–Moreau theorem in infinite dimension, for an extended-real concave functional, on LpL_pLp​ with dual LqL_qLq​. That requires Hahn–Banach separation of a closed convex hypograph and the identification of the dual of LpL_pLp​, and Mathlib provides only parts of the latter. Upper semicontinuity in the norm topology must be converted to weak semicontinuity, and the value −∞-\infty−∞ must be handled throughout. Example 2.28 of the book shows that dropping upper semicontinuity breaks the representation, so the hypothesis cannot be avoided. The restriction of the infimum to densities with EZ=1\mathbb EZ=1EZ=1, Z≥0Z\ge0Z≥0 is a separate step: one must show that every other ZZZ has A+(Z)=−∞\mathcal A^+(Z)=-\inftyA+(Z)=−∞. The first sentence of Theorem B.1 fails as printed when hhh has no continuous affine minorant, so the natural "largest l.s.c. convex minorant" route to the biconjugate needs care.

Formalization scope

Functionals are EReal-valued maps on Mathlib's Lp ℝ p P, with p ≠ ⊤, [Fact (1 ≤ p)] and [p.HolderConjugate q]. The pairing is the Bochner integral of YZYZYZ, integrable by Hölder's inequality. Conjugates are EReal suprema and infima over the whole space, so they are never a junk default. (A2), (D2) and (A4) are written as the book's inequalities in EReal, where 0⋅(±∞)=00\cdot(\pm\infty)=00⋅(±∞)=0. Non-atomicity is the book's atom definition, which is stronger than Mathlib's NoAtoms. Semicontinuity is for the norm topology. "Proper" follows the concave or convex notion of Appendix B. The book's abstract dual pair is instantiated as (Lp,Lq)(L_p,L_q)(Lp​,Lq​) with 1≤p<∞1\le p<\infty1≤p<∞, the example it gives itself.

A trivializing formalization would take the infimum in (2.11) over all of LqL_qLq​ (Fenchel–Moreau alone), or replace A+\mathcal A^+A+ by a real-valued function and so discard the −∞-\infty−∞ values that encode the constraints. The goal does neither: the infimum ranges over the densities, and A+\mathcal A^+A+ is the EReal conjugate.

Beyond the paper. There are three variants, each a corrected statement beside its faithful one:

  • deviation_representation_corrected (F1): (2.12) prints inf⁡\infinf where sup⁡\supsup is meant. For D=E−AV@R1/2\mathcal D=\mathbb E-\mathbb{AV@R}_{1/2}D=E−AV@R1/2​ and Y=±1Y=\pm1Y=±1, D(Y)=1\mathcal D(Y)=1D(Y)=1, but Z=−YZ=-YZ=−Y gives −1-1−1.
  • fenchel_moreau_largest_corrected (F2): Theorem B.1's first sentence needs h∗≢+∞h^*\not\equiv+\inftyh∗≡+∞. For h=−(EY)2h=-(\mathbb EY)^2h=−(EY)2 on {EY≥0}\{\mathbb EY\ge0\}{EY≥0}, h∗∗≡−∞h^{**}\equiv-\inftyh∗∗≡−∞ is not the largest l.s.c. convex minorant.
  • acceptabilityOfSet_properties_corrected (F3): Proposition 2.27(i) needs a monotone S\mathcal SS (a closed set built from line segments gives AS(1n1B)=2n\mathcal A_{\mathcal S}(\tfrac1n1_B)=2nAS​(n1​1B​)=2n but AS(0)=0\mathcal A_{\mathcal S}(0)=0AS​(0)=0), and (v) holds only for λ>0\lambda>0λ>0 (S=∅\mathcal S=\emptysetS=∅).

A complete development needs Fenchel–Moreau for extended-real functionals on LpL_pLp​, the duality Lp∗≅LqL_p^*\cong L_qLp∗​≅Lq​ for 1≤p<∞1\le p<\infty1≤p<∞, and coupling constructions on non-atomic spaces for version independence. All of these are reusable well beyond risk theory. Contributions of any of these pieces, or proofs of the corrected variants, are welcome.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. https://doi.org/10.1142/6478
  • P. Artzner, F. Delbaen, J.-M. Eber, D. Heath, Coherent measures of risk, Mathematical Finance 9 (1999) 203–228. https://doi.org/10.1111/1467-9965.00068
  • H. Föllmer, A. Schied, Convex measures of risk and trading constraints, Finance and Stochastics 6 (2002) 429–447. https://doi.org/10.1007/s007800200072
  • A. Ruszczyński, A. Shapiro, Optimization of convex risk functions, Mathematics of Operations Research 31 (2006) 433–452. https://doi.org/10.1287/moor.1050.0186
  • R. T. Rockafellar, Conjugate Duality and Optimization, SIAM, 1974. https://doi.org/10.1137/1.9781611970524
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Control TheoryOperations ResearchProbability+1·Captain: Shuze Chen

Stochastic Networks XV: Positive Recurrence under MaxWeight SchedulingTextbook

Scheduling shared service capacity

A switch or wireless network can have several queues ready for service while its hardware permits only certain combinations to be served together. A scheduler must choose a feasible combination repeatedly as new packets arrive. The question is whether this local sequence of decisions keeps the queue process stable whenever the arrival rates fit within the network's service capacity. Kelly and Yudovina formulate this question for finite service schedules and independent Poisson arrivals in §7.8 of Stochastic Networks.

MaxWeight scheduling gives larger queues greater influence over the choice of schedule. An exponent controls how strongly queue length affects priority. The chapter's target is a stability guarantee for every positive exponent, rather than a guarantee confined to the familiar linear weighting. The supplied Lecture Notes PDF states this as Theorem 7.13, printed page 180, and develops supporting analytic questions in Appendix D.

The queueing model

Let RRR be a finite nonempty set of queues. A schedule is a vector σ∈NR\sigma\in\mathbb N^Rσ∈NR describing how many packets each queue can serve in one time slot. The feasible schedule family SSS is finite and nonempty. It is downward closed: reducing any schedule coordinate leaves a feasible schedule. This includes the possibility of unused service when a selected queue has fewer packets than the schedule permits.

The admissible region is

Λ={v∈RR:v≥0, ∃(cσ)σ∈S, cσ≥0, ∑σ∈Scσ=1, v≤∑σ∈Scσσ}.\Lambda=\left\{v\in\mathbb R^R:v\ge0,\ \exists(c_\sigma)_{\sigma\in S},\ c_\sigma\ge0,\ \sum_{\sigma\in S}c_\sigma=1,\ v\le\sum_{\sigma\in S}c_\sigma\sigma\right\}.Λ={v∈RR:v≥0, ∃(cσ​)σ∈S​, cσ​≥0, σ∈S∑​cσ​=1, v≤σ∈S∑​cσ​σ}.

It describes arrival rates dominated by an average of feasible schedules. The interior used here is the ordinary interior in RR\mathbb R^RRR.

Fix α>0\alpha>0α>0. At queue vector qqq, a schedule is drawn from a fixed probability distribution supported on the maximizers of ∑rσrqrα\sum_r\sigma_rq_r^\alpha∑r​σr​qrα​. New arrivals ArA_rAr​ in the slot are independent Poisson variables of means λr\lambda_rλr​, independent of the scheduling randomization and the past. The next queue vector is

qr′=(qr−σr)++Ar.q'_r=(q_r-\sigma_r)^++A_r.qr′​=(qr​−σr​)++Ar​.

These laws specify a homogeneous Markov chain on the countable state space NR\mathbb N^RNR. They follow the general model in §7.8 and the explicit empty-queue convention in Example D.4, printed page 213.

Formalization targets

The goal is Theorem 7.13: for λ∈int⁡Λ\lambda\in\operatorname{int}\Lambdaλ∈intΛ, the MaxWeight-α\alphaα queue chain is positive recurrent. In return-time notation,

∀q∈NR,Eq[τq+]<∞,τq+=inf⁡{n≥1:q(n)=q}.\forall q\in\mathbb N^R,\qquad \mathbb E_q[\tau_q^+]<\infty,\qquad \tau_q^+=\inf\{n\ge1:q(n)=q\}.∀q∈NR,Eq​[τq+​]<∞,τq+​=inf{n≥1:q(n)=q}.

This retains every positive value of α\alphaα and the full queue process.

Three supporting targets are selected from the same supplied source. Proposition D.1 states the Foster–Lyapunov criterion for an irreducible countable chain and an arbitrary finite exception set. A nonnegative function with drift at most −ϵ-\epsilon−ϵ outside that set and at most b−ϵb-\epsilonb−ϵ inside it yields finite expected return to the set from every starting state and positive recurrence.

Exercise 7.18 concerns the weighted drift

D(q)=∑rqrαE[qr′−qr∣q].D(q)=\sum_rq_r^\alpha\mathbb E[q'_r-q_r\mid q].D(q)=r∑​qrα​E[qr′​−qr​∣q].

It asks for constants ϵ,K>0\epsilon,K>0ϵ,K>0 and finite bbb such that

∥q∥2>K  ⟹  D(q)<−ϵ∥q∥2α,∥q∥2≤K  ⟹  D(q)<b.\|q\|_2>K\implies D(q)<-\epsilon\|q\|_2^\alpha,\qquad \|q\|_2\le K\implies D(q)<b.∥q∥2​>K⟹D(q)<−ϵ∥q∥2α​,∥q∥2​≤K⟹D(q)<b.

Exercise D.1(3) asks for finite moments of Y=max⁡(A,B)Y=\max(A,B)Y=max(A,B), where BBB is a finite service bound and AAA is Poisson, and for the tail term

E ⁣[(∣(1+Y/K)α+1∣+1)1{Y>δK}]\mathbb E\!\left[\left(\left|(1+Y/K)^{\alpha+1}\right|+1\right)\mathbf1_{\{Y>\delta K\}}\right]E[(​(1+Y/K)α+1​+1)1{Y>δK}​]

to tend to zero as K→∞K\to\inftyK→∞ for fixed δ>0\delta>0δ>0. The source locations are printed pages 210–211, 182, and 214–215 respectively.

What the result establishes

The recurrence conclusion concerns repeated operation over an unlimited number of slots. It asserts a finite mean return time to each queue state under the specified policy. It does not require an explicit formula for the stationary distribution, nor does it prescribe a numerical delay guarantee. The result therefore identifies a capacity regime in which this queue-based scheduling rule is stable, while leaving performance within that regime as a separate question.

The formalization contribution is the connection between a concrete random scheduling transition law and recurrence on an infinite state space. Its reusable components include the capacity region of finite schedules, capped-service queue transitions, extended return expectations, and the Poisson envelope estimates. The textbook presents the theorem as an established result with a proof sketch. The theorem items here are statements awaiting proofs; compilation verifies their Lean syntax and types, not their mathematical proofs.

Where faithfulness requires care

Negative drift by itself is insufficient for the recurrence conclusion. The distinctions between negative drift, drift bounded away from zero, and control of upward increments matter in the chapter's discussion, printed pages 180–181. Arbitrary positive real exponents also require attention at empty queues and to unbounded Poisson arrivals.

The sketch's equality between actual departures and a chosen schedule fails when a positive queue is shorter than the proposed service. This is a proof gap, not a counterexample to the stability theorem. Appendix D additionally switches between conditioning on the full vector and conditioning on one coordinate in (D.5). Those conditional expectations need not agree for coupled schedules. The selected statements retain actual capped departures and avoid relying on that ambiguous display. Completing the analytic link to the goal remains part of the proof task.

Formalization scope

Queue and schedule coordinates are natural numbers, rates are nonnegative real numbers, and the exponent is an arbitrary positive real. The schedule family is a finite set of vectors. Random tie rules are stationary probability kernels supported on the maximizing schedules; the source specifies no particular distribution among ties. The norm in Exercise 7.18 is made Euclidean explicitly. Constants there are chosen before the queue vector is quantified, so they cannot depend on the current state or time.

Return times are represented by extended nonnegative sums of survival probabilities. Consequently, an event of never returning has infinite expected cost. Real drift sums have explicit absolute-integrability conditions. In the queue drift and Poisson moment items, integrability is a conclusion, not an assumed substitute for analysis. The Poisson tail term is an unconditional tail integral, including when its conditioning event would have probability zero.

No selected statement contains an unspecified O(⋅)O(\cdot)O(⋅) term or a high-probability claim; there are therefore no numerical asymptotic constants to instantiate. Exercise D.1 is included only through its explicitly numbered part (3). The remaining parts, (D.5), congestion-control optimization results, and the switch-specific matching example are outside this mission's theorem list. No variants are posed.

Stability is not defined as negative drift, and the goal is not restricted to α=1\alpha=1α=1 or a finite truncation of the queue space. Mathlib supplies probability mass functions, product measures, Poisson laws, real powers, and topology. The local definitions supply the scheduling and recurrence interfaces needed to state the targets.

Selected references

  • F. P. Kelly and E. Yudovina, Stochastic Networks, Cambridge University Press, 2014. DOI: 10.1017/CBO9781139565363. Exact indices and quotations refer to the supplied Lecture Notes on Stochastic Networks PDF, SHA-256 ec271d555059aee58613e5e9a98b8346214b16185c527314f5d94c1ac8b17b6a; correspondence with a particular published printing has not been verified.
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Convex OptimizationOperations ResearchProbability·Captain: Shuze Chen

Stochastic Networks XIII: The Capacity Region of Distributed Random AccessTextbook

Motivation

Stations sharing a communication channel must decide when to transmit. If nearby stations transmit together, their signals may interfere; if they all wait, capacity is wasted. A central scheduler can coordinate activity, but distributed access assigns decisions to individual stations. The mathematical question is whether simple random local decisions can supply all the service combinations that the interference constraints permit. This mission concerns the idealized continuous-time model in Section 5.4 of Kelly and Yudovina, Stochastic Networks, using the supplied Lecture Notes PDF.

The model isolates a capacity question from implementation issues. Stations sense active neighbors immediately, so collisions do not occur. Transmission durations and attempt clocks are exponential. The question concerns the equilibrium activity of this process for fixed parameters. Delayed sensing, packet queues, and parameter adaptation require additional results and are outside the theorem's claim.

Setting

An interference graph is a finite simple undirected graph whose vertices are stations. An edge means that its two endpoints cannot transmit together. Write RRR for the station set and SSS for the set of binary activity vectors n=(nr)r∈Rn=(n_r)_{r\in R}n=(nr​)r∈R​ satisfying this restriction. The value nr=1n_r=1nr​=1 means that station rrr is transmitting. The all-zero vector is always feasible.

Each station has a finite real parameter θr\theta_rθr​. An active station stops transmitting at rate 111. An inactive station starts at rate exp⁡(θr)\exp(\theta_r)exp(θr​) when all its neighbors are inactive. These transitions define a continuous-time Markov chain on SSS. Its generator is QQQ, with negative total outgoing rates on the diagonal, and its transition matrices are P(t)=exp⁡(tQ)P(t)=\exp(tQ)P(t)=exp(tQ) for t≥0t\ge0t≥0.

A distribution ppp on feasible schedules offers mean activity ∑np(n)nr\sum_n p(n)n_r∑n​p(n)nr​ at station rrr. The capacity region includes every nonnegative arrival vector that some such distribution can dominate:

Λ={λ≥0:∃p≥0,∑n∈Sp(n)=1,∑n∈Sp(n)nr≥λr(r∈R)}.\Lambda=\left\{\lambda\ge0:\exists p\ge0,\quad\sum_{n\in S}p(n)=1,\quad \sum_{n\in S}p(n)n_r\ge\lambda_r\quad(r\in R)\right\}.Λ={λ≥0:∃p≥0,n∈S∑​p(n)=1,n∈S∑​p(n)nr​≥λr​(r∈R)}.

This definition permits arbitrary distributions on feasible schedules. The random-access process produces a much more specific family, indexed by one real number per station.

Formalization targets

Equation (5.8) identifies the stationary distribution of the specified chain:

πθ(n)=exp⁡(∑rnrθr)∑m∈Sexp⁡(∑rmrθr),πθP(t)=πθ(t≥0).\pi_\theta(n)=\frac{\exp(\sum_r n_r\theta_r)}{\sum_{m\in S}\exp(\sum_r m_r\theta_r)}, \qquad \pi_\theta P(t)=\pi_\theta\quad(t\ge0).πθ​(n)=∑m∈S​exp(∑r​mr​θr​)exp(∑r​nr​θr​)​,πθ​P(t)=πθ​(t≥0).

The goal is Theorem 5.17, printed page 126 of the supplied PDF. Every arrival vector in the ordinary interior of Λ\LambdaΛ has strictly smaller coordinates than the equilibrium service vector for some finite parameters:

λ∈int⁡Λ⟹∃θ∈RR,λr<∑n∈Snrπθ(n)(r∈R).\lambda\in\operatorname{int}\Lambda \quad\Longrightarrow\quad \exists\theta\in\mathbb R^R,\quad \lambda_r<\sum_{n\in S}n_r\pi_\theta(n)\quad(r\in R).λ∈intΛ⟹∃θ∈RR,λr​<n∈S∑​nr​πθ​(n)(r∈R).

Three Appendix C milestones supply the accompanying optimization statements. For a convex objective fff and componentwise convex constraint map hhh on a convex set XXX, Theorem C.7 asserts convexity of the extended value function ϕ(b)=inf⁡{f(x):x∈X,h(x)≤b}\phi(b)=\inf\{f(x):x\in X,h(x)\le b\}ϕ(b)=inf{f(x):x∈X,h(x)≤b}. Theorem C.3 supplies a nonvertical support at an interior point of its finite-value domain. Theorem C.4 states the equivalence between such support and the strong Lagrangian principle for equality constraints, with

Lb(x;y)=f(x)+yT(b−h(x)),ϕ(b)=inf⁡x∈XLb(x;y).L_b(x;y)=f(x)+y^T(b-h(x)),\qquad \phi(b)=\inf_{x\in X}L_b(x;y).Lb​(x;y)=f(x)+yT(b−h(x)),ϕ(b)=x∈Xinf​Lb​(x;y).

The faithful C.4 statement is retained without an unprinted finiteness hypothesis. Its infinite-value defect and the separately labelled correction are described below. The goal itself retains the source's strict service inequalities.

Significance

The capacity theorem says that the exponential random-access family does not leave a gap inside the region attainable by arbitrary mixtures of independent schedules. It provides a service margin in every coordinate at once. Its quantifiers allow the parameters to depend on the graph and arrival vector, but require every parameter to remain a finite real number. The theorem does not provide a uniform parameter bound as the arrival vector approaches the boundary.

The known mathematical result is attributed to Jiang and Walrand in the supplied source. The formalization target is a checked statement of that result and its supporting mathematical interfaces. The proposal's theorem declarations remain proof tasks. The finite exclusion process, its invariant law, and the distinction between feasible schedule mixtures and exponential-family marginals are reusable in later work on scheduling. The extended-value optimization layer can also support problems unrelated to communication networks.

Difficulty

Normalizing positive exponential weights only constructs a probability distribution. It does not establish that the distribution is invariant under the given dynamics, nor that its marginal vectors cover every strictly feasible demand. Changing one station's parameter changes the other stations' equilibrium opportunities through interference. Coordinatewise scalar tuning therefore does not settle simultaneous coverage.

The optimization statements require care at infeasible and unbounded problems. A real-valued infimum with a default value would conceal these cases. In particular, the literal C.4 equivalence fails for an empty domain: both primal and Lagrangian infima are +∞+\infty+∞, but no finite-height hyperplane touches that value. This is an issue with the unrestricted statement, not a new hypothesis for the capacity theorem.

Formalization scope

Stations are indexed by Fin d, and activity coordinates by Fin 2. Simple graphs enforce symmetry and exclude self-interference. A decidability instance is computational bookkeeping for a finite adjacency relation. The empty station set is permitted: it has one empty schedule, and the service conclusion has no coordinates. For one station the mean activity is exp⁡(θ)/(1+exp⁡(θ))\exp(\theta)/(1+\exp(\theta))exp(θ)/(1+exp(θ)). All normalizing sums are finite and strictly positive because the empty schedule contributes weight one.

Interior means ambient Euclidean interior. Arrival vectors in the closed region alone are insufficient: at the one-station boundary demand λ=1\lambda=1λ=1, no finite parameter supplies service greater than one. Finding F1 records this sharpness example; no extra sharpness item is posed.

The CTMC is represented by its finite generator and matrix-exponential transition semigroup. Its stationary-law theorem asserts invariance for every nonnegative time. Optimization infima use EReal, so infeasibility gives +∞+\infty+∞ and unboundedness below gives −∞-\infty−∞. Convexity is expressed through the real epigraph; supporting affine functions have real heights and slopes. Slack elimination in (C.2) preserves the inequality h(x)≤bh(x)\le bh(x)≤b. No asymptotic constants or failure probabilities require instantiation in these targets.

Beyond the paper. The single corrected variant of C.4 adds exactly that ϕ(b)\phi(b)ϕ(b) is finite. Finding F2 gives the empty-domain counterexample to the unrestricted equivalence and the supporting argument for the correction. The original remains the milestone anchor. Findings F3 and F4 separately record the slack-multiplier sign error on printed page 209 and the word “maximized” in the minimization argument on printed page 127; neither changes the goal or creates a variant.

The definitions have concrete mathematical bodies without proof placeholders. The theorem types expose their defining formulas for independent auditing, and use Mathlib's finite sums, graph types, topology, convexity, extended reals, and matrix exponential. A formulation that assumes the desired service vector or proves only normalization would not capture this mission.

Selected references

  • F. P. Kelly and E. Yudovina, Stochastic Networks, Cambridge University Press, 2014. DOI. All numbered claims and page citations refer to the supplied Lecture Notes on Stochastic Networks PDF: Section 5.4, printed pages 125–128 (PDF pages 133–136), and Appendix C, printed pages 207–209 (PDF pages 215–217). Equivalence of this supplied file to a particular published printing is unverified.
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Algorithmic Game TheoryEconomicsOperations Research·Captain: Shuze Chen

Impact of Traceability Technology Adoption in Food Supply Chain Networks: Under the Break Point Criterion, Traceability Lowers the Retailer's Equilibrium Profit Exactly on an Interval (r₁, r₂)Research Paper

Motivation

Food-borne outbreaks are traced slowly: when contaminated produce reaches shelves, the source is often unknown for weeks, and retailers recall everything. Traceability technology (for example blockchain ledgers) identifies the contaminated source at once, so only its units are discarded. Regulators and large retailers have pushed for it, and the intuitive view is that every member of the chain gains. Dong, Jiang & Xu (Management Science, 2022) show in a three-tier pricing game that this is not so: the chain's most powerful member, the retailer, can earn less in equilibrium with traceability than without it. The reversal happens for an explicit interval of retail prices, under an explicit condition on the primitives.

Setting

A retailer sells n≥2n \ge 2n≥2 units at an exogenous retail price rrr. She buys them at a wholesale price www from one tier-1 supplier, who buys one unit at a procurement price ppp from each of nnn tier-2 suppliers (farms). Each farm produces at unit cost cp>0c_p > 0cp​>0 and is contaminated independently with probability ρ\rhoρ, or ρe\rho_eρe​ if it exerts a risk-reduction effort at cost e>0e > 0e>0, where 0≤ρe<ρ<10 \le \rho_e < \rho < 10≤ρe​<ρ<1 and ρτ=ρ−ρe\rho_\tau = \rho - \rho_eρτ​=ρ−ρe​. Assumption 1 of the paper is cp<cˉp=(1−ρ)e/ρτc_p < \bar c_p = (1-\rho)e/\rho_\taucp​<cˉp​=(1−ρ)e/ρτ​. A farm's survival probability is s=1−ρes = 1-\rho_es=1−ρe​ with effort and 1−ρ1-\rho1−ρ without.

  • Case N (no traceability). Any contamination voids every payment. Farm iii's payoff under an effort profile aaa is (∏js(aj))p−(e1{ai}+cp)\big(\prod_j s(a_j)\big)p - (e\mathbb 1\{a_i\} + c_p)(∏j​s(aj​))p−(e1{ai​}+cp​).
  • Case T (traceability). Only contaminated units are lost. Farm iii's payoff is s(ai)p−(e1{ai}+cp)s(a_i)p - (e\mathbb 1\{a_i\} + c_p)s(ai​)p−(e1{ai​}+cp​).

Tier-1 earns (expected units sold)⋅(w−p)\cdot(w-p)⋅(w−p) and the retailer (expected units sold)⋅(r−w)\cdot(r-w)⋅(r−w); expected units sold are n∏js(aj)n\prod_j s(a_j)n∏j​s(aj​) in Case N and ∑js(aj)\sum_j s(a_j)∑j​s(aj​) in Case T. The retailer chooses www, tier-1 then ppp, and the farms then choose effort simultaneously. The solution concept is subgame-perfect Nash equilibrium (SPNE) with the paper's selection rules: the Pareto-dominant tier-2 equilibrium is played; an indifferent farm exerts effort; an indifferent tier-1 or retailer induces effort; an agent with zero profit still trades.

The paper solves both games in closed form. With ℓ=(1−ρe)n−(1−ρ)n\ell = (1-\rho_e)^n - (1-\rho)^nℓ=(1−ρe​)n−(1−ρ)n, the effort thresholds of the retail price are

rNe=max⁡{(1−ρe)n+1e−[2(1−ρe)n−(1−ρ)n]ρτcpρτℓ2, eρτ(1−ρe)n−1},rTe=(1−ρe)2e−(1+ρ−2ρe)ρτcpρτ3,r^e_N = \max\Big\{\tfrac{(1-\rho_e)^{n+1}e-[2(1-\rho_e)^n-(1-\rho)^n]\rho_\tau c_p}{\rho_\tau\ell^2},\ \tfrac{e}{\rho_\tau(1-\rho_e)^{n-1}}\Big\},\qquad r^e_T = \tfrac{(1-\rho_e)^2e-(1+\rho-2\rho_e)\rho_\tau c_p}{\rho_\tau^3},rNe​=max{ρτ​ℓ2(1−ρe​)n+1e−[2(1−ρe​)n−(1−ρ)n]ρτ​cp​​, ρτ​(1−ρe​)n−1e​},rTe​=ρτ3​(1−ρe​)2e−(1+ρ−2ρe​)ρτ​cp​​,

and the retailer's profit on the relevant branches (Tables EC.1–EC.2) is π0Ne(r)=n(1−ρe)n(r−wNe)\pi^e_{0N}(r) = n(1-\rho_e)^n(r - w^e_N)π0Ne​(r)=n(1−ρe​)n(r−wNe​), π0To(r)=n(1−ρ)r−ncp\pi^o_{0T}(r) = n(1-\rho)r - nc_pπ0To​(r)=n(1−ρ)r−ncp​ and π0Te(r)=n(1−ρe)(r−wTe)\pi^e_{0T}(r) = n(1-\rho_e)(r - w^e_T)π0Te​(r)=n(1−ρe​)(r−wTe​), with wNe=max⁡{(1−ρe)e−ρτcpρτℓ,eρτ(1−ρe)n−1}w^e_N = \max\{\frac{(1-\rho_e)e-\rho_\tau c_p}{\rho_\tau\ell}, \frac{e}{\rho_\tau(1-\rho_e)^{n-1}}\}wNe​=max{ρτ​ℓ(1−ρe​)e−ρτ​cp​​,ρτ​(1−ρe​)n−1e​} and wTe=(1−ρe)e−ρτcpρτ2w^e_T = \frac{(1-\rho_e)e-\rho_\tau c_p}{\rho_\tau^2}wTe​=ρτ2​(1−ρe​)e−ρτ​cp​​. The paper's Definition 1:

DEFINITION 1 (BREAK POINT CRITERION). The Break Point Criterion (BPC) is satisfied if traceability adoption decreases the retailer's equilibrium profit when the retail price is at the effort threshold with traceability, i.e., π0Te(rTe)<π0Ne(rTe)\pi^e_{0T}(r^e_T) < \pi^e_{0N}(r^e_T)π0Te​(rTe​)<π0Ne​(rTe​).

Formalization targets

Goal: Proposition 3 (p. 21)

Under the standing assumptions and BPC there exist r1,r2r_1, r_2r1​,r2​ with

rNe<r1<rTe<r2,π0To(r1)=π0Ne(r1),π0Te(r2)=π0Ne(r2),r^e_N < r_1 < r^e_T < r_2,\qquad \pi^o_{0T}(r_1) = \pi^e_{0N}(r_1),\qquad \pi^e_{0T}(r_2) = \pi^e_{0N}(r_2),rNe​<r1​<rTe​<r2​,π0To​(r1​)=π0Ne​(r1​),π0Te​(r2​)=π0Ne​(r2​),

such that both games have an SPNE at every retail price, and for all SPNE sNs_NsN​, sTs_TsT​ at rrr,

r1<r<r2  ⟹  ΠT(r;sT)<ΠN(r;sN),r∉(r1,r2)  ⟹  ΠN(r;sN)≤ΠT(r;sT),r_1 < r < r_2 \implies \Pi_T(r; s_T) < \Pi_N(r; s_N),\qquad r \notin (r_1, r_2) \implies \Pi_N(r; s_N) \le \Pi_T(r; s_T),r1​<r<r2​⟹ΠT​(r;sT​)<ΠN​(r;sN​),r∈/(r1​,r2​)⟹ΠN​(r;sN​)≤ΠT​(r;sT​),

where ΠN\Pi_NΠN​, ΠT\Pi_TΠT​ are the retailer's equilibrium profits.

Milestones

In proof order: Lemma 1 (tier-2 equilibrium, Case N, p. 9); Lemma 2 (tier-1's optimal price, Case N, p. 10); Proposition 1 (SPNE, Case N, p. 11); Lemma 3, Lemma 4 (Case T, p. 13); Proposition 2 (SPNE, Case T, p. 14); Lemma 5 (BPC implies rNe<rTer^e_N < r^e_TrNe​<rTe​ and (1−ρe)n>1−ρ(1-\rho_e)^n > 1-\rho(1−ρe​)n>1−ρ, p. 21).

Stronger: the exact sign pattern

The variant proposition_3_strong adds strict increase with traceability on (rTo,r1)∪(r2,∞)(r^o_T, r_1) \cup (r_2, \infty)(rTo​,r1​)∪(r2​,∞), where rTo=cp/(1−ρ)r^o_T = c_p/(1-\rho)rTo​=cp​/(1−ρ), and equality on (−∞,rTo]∪{r1,r2}(-\infty, r^o_T] \cup \{r_1, r_2\}(−∞,rTo​]∪{r1​,r2​}.

Significance

Proposition 3 is the paper's headline result (Abstract, p. 1): removing the cascade threat does not make every member better off, and the losses concentrate on retail prices around the traceability effort threshold rTer^e_TrTe​. It underlies the paper's later welfare discussion (Observation 1, Proposition 4), where every member is worse off on part of the interval, and the policy point that adoption may need subsidies or contract adjustments.

The result is proved in the paper, partly in sketch form; none of it is formalized. A formal development produces the first fully specified multi-tier pricing-and-effort game on the platform: an nnn-player effort game with a selection rule, two nested best-response problems with tie rules, and subgame-perfect equilibrium as a predicate, together with a welfare comparison stated on equilibria rather than on formulas.

Difficulty

Each step is elementary, but the equilibrium has to be established, not assumed. The tier-2 stage is an nnn-player game in Case N whose equilibria above pNep^e_NpNe​ can be multiple (a stag hunt), so the selection rule matters. Tier-1 and the retailer optimize a margin whose effect on effort is a step function of the price; their maxima are attained only because the thresholds are closed and the tie rules settle the boundary, and they must be identified among all real prices. The final comparison is between two piecewise-linear functions with different breakpoints in the two cost branches. The paper prints no proof of Lemma 5, Lemma 4 or Proposition 2, and Proposition 3's printed proof is a short sketch that treats the high-cost branch as "similar".

Formalization scope

Everything lives in the namespace FoodTrace.Adoption (definition module Def_FoodTrace_Adoption_Model). Conventions:

  • Parameters Params = (n, ρ, ρe, e, cp); Standing collects n≥2n \ge 2n≥2, 0≤ρe0 \le \rho_e0≤ρe​, ρe<ρ\rho_e < \rhoρe​<ρ, ρ<1\rho < 1ρ<1, e>0e > 0e>0, cp>0c_p > 0cp​>0 and Assumption 1. The implicit hypotheses 0≤ρe0 \le \rho_e0≤ρe​, ρ<1\rho < 1ρ<1, e>0e > 0e>0, cp>0c_p > 0cp​>0 are made explicit.
  • Effort is a Bool per farm; profiles are Fin n → Bool, with no symmetry built in.
  • A viable tier-2 equilibrium follows (EC.9) of p. ec22: nonnegative payoffs; effort weakly preferred by farms exerting it; no effort strictly preferred by the others. The selected outcome weakly Pareto-dominates every viable equilibrium; "no sale" is selected exactly when none exists.
  • "No trade" is none with profit 0; prices range over all of R\mathbb RR.
  • Best responses and retailer optimality are maximizers over all prices and no trade, with the tie rules as explicit clauses (induce effort, then trade, whenever some maximizer does).
  • Case T revenue for asymmetric profiles is ∑js(aj)\sum_j s(a_j)∑j​s(aj​) times the margin; the paper prints only the symmetric case.
  • wNew^e_NwNe​ and rNer^e_NrNe​ carry the max, so π0Ne\pi^e_{0N}π0Ne​ is one formula in both cost branches. c‾p\underline c_pc​p​ is cpLow, cˉp\bar c_pcˉp​ is cpBar.
  • Proposition 3's "Otherwise, traceability adoption increases the retailer's profit" is stated as ΠN≤ΠT\Pi_N \le \Pi_TΠN​≤ΠT​: the profits are equal at r1r_1r1​, r2r_2r2​ and for r≤rTor \le r^o_Tr≤rTo​.

The retailer's profit in the goal is her payoff at an SPNE of the game, not the closed forms of Tables EC.1–EC.2; the goal asserts the existence of SPNE in both games at every retail price, so the comparison over all equilibria is not vacuous; and BPC is satisfiable (the Figure 4 instance n=2n = 2n=2, ρ=0.4\rho = 0.4ρ=0.4, ρe=0.1\rho_e = 0.1ρe​=0.1, cp=e=0.4c_p = e = 0.4cp​=e=0.4 gives π0Te(rTe)=36/5<198/25=π0Ne(rTe)\pi^e_{0T}(r^e_T) = 36/5 < 198/25 = \pi^e_{0N}(r^e_T)π0Te​(rTe​)=36/5<198/25=π0Ne​(rTe​)).

Beyond the paper. One variant is posed beside the faithful goal: proposition_3_strong (strengthened, finding F2), the exact sign pattern above. Evidence: a four-region comparison of the equilibrium profits, confirmed at 1.87 million sampled retail prices on 18,820 random BPC instances in both cost branches.

Needed infrastructure: finite products and sums over Fin n, real inequalities with powers, and case analysis on Option. The equilibrium layer (selection, best responses with tie rules, SPNE as a predicate) is reusable for other sequential supply-chain games. Proofs of the stage results (Lemmas 1–4, Propositions 1–2) and of Lemma 5 are welcome as independent contributions.

Selected references

  • Y. Dong, B. Jiang, M. Xu, Impact of Traceability Technology Adoption in Food Supply Chain Networks, Management Science, 2022. https://doi.org/10.1287/mnsc.2022.4440 (accepted manuscript: SSRN 3484664, https://ssrn.com/abstract=3484664)
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Algorithmic Game TheoryEconomicsOperations Research+1·Captain: Shuze Chen

Food Delivery Service and Restaurant: Friend or Foe?: With Convenient Delivery, a Critical Mass of Tech-Savvy Customers Makes the Restaurant Delivery-Only and Cuts Platform Profit and WelfareResearch Paper

Motivation

Food delivery platforms such as Uber Eats, DoorDash and Meituan let a restaurant serve customers who never enter it, but they also charge those customers a delivery fee and share the restaurant's kitchen with its walk-in trade. Whether the platform helps or hurts the restaurant is a question restaurant owners, platforms and regulators all ask. Chen, Hu and Wang (Management Science, 2022) answer it in a stylized game: a restaurant whose kitchen is a queue, a platform that sets a fee, and two kinds of customers who decide where to eat by comparing expected waiting costs. Their first main result, Proposition 1, describes how the equilibrium changes as more customers become able to order through the platform: below a critical mass nothing changes for the restaurant, and at the critical mass the restaurant abruptly turns into a delivery-only kitchen. The analysis builds on the unobservable-queue joining games of Edelson and Hilderbrand (1975) and Hassin and Haviv (2003).

Setting

A kitchen serves meals at rate μ>0\mu>0μ>0. At total joining rate λ<μ\lambda<\muλ<μ the expected wait for food is 1/(μ−λ)1/(\mu-\lambda)1/(μ−λ). A meal is worth RRR to a customer. Walk-in customers pay the food price ppp and incur waiting cost rate c>0c>0c>0; food-delivery customers pay ppp plus the delivery fee θ\thetaθ and incur the smaller waiting cost rate ϕ∈[0,c)\phi\in[0,c)ϕ∈[0,c). Their expected utilities are

UW(λ)=R−p−cμ−λ,UD(λ)=R−p−θ−ϕμ−λ,U_W(\lambda)=R-p-\frac{c}{\mu-\lambda},\qquad U_D(\lambda)=R-p-\theta-\frac{\phi}{\mu-\lambda},UW​(λ)=R−p−μ−λc​,UD​(λ)=R−p−θ−μ−λϕ​,

and balking gives 000. Tech-savvy customers arrive at rate Λ1∈(0,μ)\Lambda_1\in(0,\mu)Λ1​∈(0,μ) and may walk in, use delivery or balk; traditional customers arrive at rate Λ0≥μ\Lambda_0\ge\muΛ0​≥μ and may walk in or balk. The delivery-worker pool is unlimited and costless.

A customers' equilibrium under (p,θ)(p,\theta)(p,θ) is a profile of joining rates (λD,λ1W,λ0W)(\lambda_D,\lambda_{1W},\lambda_{0W})(λD​,λ1W​,λ0W​) with λ=λD+λ1W+λ0W<μ\lambda=\lambda_D+\lambda_{1W}+\lambda_{0W}<\muλ=λD​+λ1W​+λ0W​<μ in which every option used by a positive rate is a best reply at λ\lambdaλ, and an arrival stream that does not fully join is no better off joining. Ties between delivery and walking in at UD=UW≥0U_D=U_W\ge0UD​=UW​≥0 go to delivery. The game has three stages. The restaurant sets p≥0p\ge0p≥0. The platform then sets θ≥0\theta\ge0θ≥0 to maximize π=θλD\pi=\theta\lambda_Dπ=θλD​. Finally customers play an equilibrium. The restaurant maximizes Π=p(λD+λW)\Pi=p(\lambda_D+\lambda_W)Π=p(λD​+λW​), where λW=λ0W+λ1W\lambda_W=\lambda_{0W}+\lambda_{1W}λW​=λ0W​+λ1W​. A subgame-perfect equilibrium (SPE) combines a customers' equilibrium after every (p,θ)(p,\theta)(p,θ), a best-response fee after every ppp, and an optimal price p∗p^*p∗. Its outcome is p∗p^*p∗, θ∗\theta^*θ∗, λD∗\lambda^*_DλD∗​, λW∗\lambda^*_WλW∗​, Π∗\Pi^*Π∗, π∗\pi^*π∗ and the social welfare S∗=Π∗+π∗+λD∗UD+λW∗UWS^*=\Pi^*+\pi^*+\lambda^*_DU_D+\lambda^*_WU_WS∗=Π∗+π∗+λD∗​UD​+λW∗​UW​, the total surplus of all stakeholders.

Formalization targets

Goal: Proposition 1 (p. 8)

Assume μ>0\mu>0μ>0, c>0c>0c>0, c<Rμc<R\muc<Rμ, Λ0≥μ\Lambda_0\ge\muΛ0​≥μ. There is ϕ1\phi_1ϕ1​ such that for every ϕ∈[0,c)\phi\in[0,c)ϕ∈[0,c) there are λ1∈(0,μ)\lambda_1\in(0,\mu)λ1​∈(0,μ) and an SPE for every Λ1∈(0,μ)\Lambda_1\in(0,\mu)Λ1​∈(0,μ) whose outcome, viewed as a function of Λ1\Lambda_1Λ1​, satisfies the following. With I=(0,μ)I=(0,\mu)I=(0,μ) if ϕ>ϕ1\phi>\phi_1ϕ>ϕ1​ and I=(0,λ1]I=(0,\lambda_1]I=(0,λ1​] otherwise:

  1. on III, p∗p^*p∗ and λD∗+λW∗\lambda^*_D+\lambda^*_WλD∗​+λW∗​ are constant, and π∗\pi^*π∗, S∗S^*S∗, λD∗\lambda^*_DλD∗​, −λW∗-\lambda^*_W−λW∗​ are weakly increasing;
  2. if ϕ≤ϕ1\phi\le\phi_1ϕ≤ϕ1​,
p∗(a)<p∗(b)  (a≤λ1<b),π∗(λ1)>lim⁡Λ1↘λ1π∗,S∗(λ1)>lim⁡Λ1↘λ1S∗;p^*(a)<p^*(b)\ \ (a\le\lambda_1<b),\qquad \pi^*(\lambda_1)>\lim_{\Lambda_1\searrow\lambda_1}\pi^*,\qquad S^*(\lambda_1)>\lim_{\Lambda_1\searrow\lambda_1}S^*;p∗(a)<p∗(b)  (a≤λ1​<b),π∗(λ1​)>Λ1​↘λ1​lim​π∗,S∗(λ1​)>Λ1​↘λ1​lim​S∗;
  1. if ϕ<c/(2Rμ/c−1)\phi<c/(2\sqrt{R\mu/c}-1)ϕ<c/(2Rμ/c​−1), then c/(2Rμ/c−1)≤ϕ1c/(2\sqrt{R\mu/c}-1)\le\phi_1c/(2Rμ/c​−1)≤ϕ1​ and λD∗+λW∗\lambda^*_D+\lambda^*_WλD∗​+λW∗​ on (0,λ1](0,\lambda_1](0,λ1​] is below its limit as Λ1↗μ\Lambda_1\nearrow\muΛ1​↗μ.

The thresholds are existential, as printed. The milestones pin them to the values the proof constructs: χ\chiχ is the root of −Rχ3−μϕχ+2μ2ϕ-R\chi^3-\mu\phi\chi+2\mu^2\phi−Rχ3−μϕχ+2μ2ϕ in [0,μ][0,\mu][0,μ], λ2=μ−χ\lambda_2=\mu-\chiλ2​=μ−χ, λ1\lambda_1λ1​ is the smallest root of λ(R−μϕ/(μ−λ)2)=(Rμ−c)2\lambda(R-\mu\phi/(\mu-\lambda)^2)=(\sqrt{R\mu}-\sqrt c)^2λ(R−μϕ/(μ−λ)2)=(Rμ​−c​)2, and ϕ1\phi_1ϕ1​ has a closed form (Online Appendix p. 23).

Milestones

The paper's own chain (Online Appendix C.1): Lemma C.2 (customers' equilibrium), Proposition C.3 (platform's best response), Corollary C.2 (restaurant's profit curve), Lemmas C.6–C.8 (the three profit curves, their maxima and intersections), Proposition C.4 (restaurant's optimal price), and Corollaries C.3–C.4 (platform profit and welfare in equilibrium). "We have Proposition 1 from Proposition C.4, Corollary C.3 and Corollary C.4."

Significance

The result separates two regimes. In the delivery-irrelevant regime, more tech-savvy customers only change who eats at the restaurant; the price and the throughput are fixed while the platform's profit and welfare grow. Past the critical mass λ1\lambda_1λ1​, the restaurant raises its price and serves only delivery customers, and the platform's profit and social welfare drop. This is the basis of the paper's answer to "friend or foe" and of its later analysis of revenue-sharing contracts that restore coordination (Proposition 2, not part of this mission).

The paper's proof is a long chain of case analyses over piecewise-defined profit functions, spread over 22 pages of appendix. A machine-checked version settles every boundary case. Reading the proof closely has already turned up several (findings F1–F9): ties in the restaurant's optimum at Λ1=λ1\Lambda_1=\lambda_1Λ1​=λ1​ and at ϕ=ϕ1\phi=\phi_1ϕ=ϕ1​; table rows that are wrong outside their derived price range; an implicit hypothesis c<Rμc<R\muc<Rμ; the degenerate case ϕ=0\phi=0ϕ=0; a tie rule that needs a precise reading; and a boundary error in Lemma C.7(3). The definitions of the queue-joining equilibrium and the three-stage Stackelberg game can be reused for other platform and queueing games. None of this has been formalized before.

Difficulty

The equilibrium is defined by optimality conditions, so each stage needs an existence-and-characterization argument, not a formula check. The customers' stage has mixed strategies with three utility comparisons and a tie rule. The platform's profit is piecewise in θ\thetaθ, with branches that switch depending on ppp and on whether Λ1≶c−ϕcμ\Lambda_1\lessgtr\frac{c-\phi}{c}\muΛ1​≶cc−ϕ​μ. The restaurant's profit is the upper envelope of three curves whose maxima must be compared through the cubic defining χ\chiχ and a quartic-type equation defining λ1\lambda_1λ1​. The obvious approach, substituting the tables, fails at the boundaries. At Λ1=λ1\Lambda_1=\lambda_1Λ1​=λ1​ and at ϕ=ϕ1\phi=\phi_1ϕ=ϕ1​ the restaurant has two optimal prices with different platform profits, so "the" equilibrium price is not unique. The jump statements are therefore about a particular equilibrium selection and about one-sided limits.

Formalization scope

All objects live in FoodDeliv.Decentral, with one definitions file, FoodDeliv_Decentral_Model. Conventions:

  • Parameters are real; the standing assumptions are μ>0\mu>0μ>0, c>0c>0c>0, 0≤ϕ<c0\le\phi<c0≤ϕ<c, Λ0≥μ\Lambda_0\ge\muΛ0​≥μ, 0<Λ1<μ0<\Lambda_1<\mu0<Λ1​<μ (the paper's focus, Online Appendix p. 7), and c<Rμc<R\muc<Rμ, which the paper uses ("Rμ/c>1R\mu/c>1Rμ/c>1") without stating it.
  • Prices and fees range over p≥0p\ge0p≥0, θ≥0\theta\ge0θ≥0.
  • The tie rule reads: at UD=UW≥0U_D=U_W\ge0UD​=UW​≥0 no tech-savvy customer walks in, and none balks while traditional customers walk in.
  • S∗S^*S∗ includes the customers' surplus. The equilibrium is defined by optimality conditions, never by the paper's tables. λ1∈(0,μ)\lambda_1\in(0,\mu)λ1​∈(0,μ), and an SPE is required at λ1\lambda_1λ1​ itself. The jumps compare the value at λ1\lambda_1λ1​ with the right limit, and every limit is asserted to exist.
  • "p∗p^*p∗" in the goal is read existentially, as an SPE selection, because of the ties; in Proposition C.4 it is read as "the table's price is optimal". Proposition 1 keeps ϕ=0\phi=0ϕ=0. The milestones about a fixed ϕ\phiϕ assume ϕ>0\phi>0ϕ>0, because at ϕ=0\phi=0ϕ=0 the delivery utility does not depend on congestion and the demand under some fees is not determined.
  • Lemma C.2's last row and Corollary C.2's last rows are stated on the price range the paper derives them for. Lemma C.7 omits item 3 and Lemma C.8 omits item 2.

Beyond the paper. No variant items are posed. The findings file records the evidence for each deviation above.

Contributions welcome: proofs of the milestones in any order; existence of customers' equilibria for every (p,θ)(p,\theta)(p,θ) under the tie rule; reusable lemmas on unimodal functions, cubic roots and one-sided limits of piecewise functions.

Selected references

  • M. Chen, M. Hu, J. Wang, Food Delivery Service and Restaurant: Friend or Foe?, Management Science, 2022. https://doi.org/10.1287/mnsc.2021.4245 (author version: SSRN 3469971, https://ssrn.com/abstract=3469971)
  • N. M. Edelson, D. K. Hilderbrand, Congestion Tolls for Poisson Queuing Processes, Econometrica 43(1), 1975. https://doi.org/10.2307/1911385
  • R. Hassin, M. Haviv, To Queue or Not to Queue: Equilibrium Behavior in Queueing Systems, Springer, 2003. https://doi.org/10.1007/978-1-4615-0359-0
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Robust Optimization XIII: Exact Quadratic Decision Rules on EllipsoidsTextbook

Decisions made with partial information

An adjustable decision is a rule that responds to information revealed after an optimization problem is specified. In production planning, for example, a later quantity may depend on observed demand, while an earlier commitment must remain constant. A robust counterpart requires the resulting decisions to satisfy the constraints for every realization in a prescribed uncertainty set. The information available to each decision is part of the model: observing one linear combination of uncertain data does not permit a policy to use all the data coordinates.

Quadratic rules provide a finite family of responses with more flexibility than affine rules. The resulting robust constraints still quantify over infinitely many uncertain realizations. This mission concerns the case in which that infinite family has an exact finite semidefinite representation: fixed recourse and ellipsoidal uncertainty, as stated in Corollary 14.3.8 of Ben-Tal, El Ghaoui and Nemirovski. The result is about optimization over the selected quadratic rules; it makes no claim that these rules attain the best value among all possible responses.

The model and the information available to a policy

Let z∈RLz\in\mathbb R^Lz∈RL denote the uncertain data and let

Z={z:∥Qz∥2≤1},Q∈Rr×L,ker⁡Q={0}.Z=\{z:\|Qz\|_2\le1\},\qquad Q\in\mathbb R^{r\times L},\quad\ker Q=\{0\}.Z={z:∥Qz∥2​≤1},Q∈Rr×L,kerQ={0}.

The uncertain linear problem has nnn decision variables and mmm constraint rows:

min⁡x{c(z)Tx+d(z):A(z)x≥b(z)}.\min_x\{c(z)^Tx+d(z):A(z)x\ge b(z)\}.xmin​{c(z)Tx+d(z):A(z)x≥b(z)}.

All four data functions are affine in zzz. For variable jjj, a specified matrix Pj∈Rkj×LP_j\in\mathbb R^{k_j\times L}Pj​∈Rkj​×L determines its observations. A quadratic decision rule has the form

Xj(z)=pj+qjTPjz+(Pjz)TRj(Pjz).X_j(z)=p_j+q_j^TP_jz+(P_jz)^TR_j(P_jz).Xj​(z)=pj​+qjT​Pj​z+(Pj​z)TRj​(Pj​z).

The optimization variables are the coefficients pj,qj,Rjp_j,q_j,R_jpj​,qj​,Rj​ and an objective threshold ttt. The matrices PjP_jPj​ are fixed data. The coefficient matrices RjR_jRj​ are unrestricted: using full arrays retains every quadratic polynomial, with harmless redundancy in their skew-symmetric parts. If Pj=0P_j=0Pj​=0, the policy is constant.

Fixed recourse means that whenever Pj≠0P_j\ne0Pj​=0, both cj(z)c_j(z)cj​(z) and column Aj(z)A_j(z)Aj​(z) are independent of zzz. Coefficients of nonadjustable variables may still be uncertain. This is Definition 14.3.1, printed p. 371, including the condition on the objective. Robust epigraph feasibility means that A(z)X(z)≥b(z)A(z)X(z)\ge b(z)A(z)X(z)≥b(z) and c(z)TX(z)+d(z)≤tc(z)^TX(z)+d(z)\le tc(z)TX(z)+d(z)≤t hold for every z∈Zz\in Zz∈Z.

Formalization targets

The supporting geometric target is Lemma 14.3.7, printed p. 384. The quadratic lift of zzz is the symmetric matrix with top-left entry zero, first column [0;z][0;z][0;z], and lower-right block zzTzz^TzzT. Its ordinary convex hull is compact and satisfies

conv⁡{[0zTzzzT]:z∈Z}={[0vTvW]:[1vTvW]⪰0, Tr⁡(QWQT)≤1}.\operatorname{conv}\left\{\begin{bmatrix}0&z^T\\z&zz^T\end{bmatrix}:z\in Z\right\} =\left\{\begin{bmatrix}0&v^T\\v&W\end{bmatrix}:\begin{bmatrix}1&v^T\\v&W\end{bmatrix}\succeq0,\ \operatorname{Tr}(QWQ^T)\le1\right\}.conv{[0z​zTzzT​]:z∈Z}={[0v​vTW​]:[1v​vTW​]⪰0, Tr(QWQT)≤1}.

The goal is Corollary 14.3.8. For every policy coefficient vector and threshold, robust epigraph feasibility is equivalent to feasibility of the explicit SDP after adding one nonnegative multiplier for each constraint row and one for the objective row. If the signed slack in row iii is written αi+βiTz+zTΓiz\alpha_i+\beta_i^Tz+z^T\Gamma_i zαi​+βiT​z+zTΓi​z, its matrix constraint is

[αi−λiβiT/2βi/2Γi+λiQTQ]⪰0,λi≥0.\begin{bmatrix}\alpha_i-\lambda_i&\beta_i^T/2\\\beta_i/2&\Gamma_i+\lambda_iQ^TQ\end{bmatrix}\succeq0,\qquad\lambda_i\ge0.[αi​−λi​βi​/2​βiT​/2Γi​+λi​QTQ​]⪰0,λi​≥0.

The model defines these coefficients directly from the original data and the observation matrices. The theorem also asserts that the matrices depend affinely on the SDP decision vector. There are m+1m+1m+1 matrix constraints of order L+1L+1L+1, and

N=1+∑j(1+kj+kj2)+(m+1)N=1+\sum_j(1+k_j+k_j^2)+(m+1)N=1+j∑​(1+kj​+kj2​)+(m+1)

scalar decision variables. With K=∑jkjK=\sum_jk_jK=∑j​kj​, the bound N≤1+n(1+K+K2)+(m+1)N\le1+n(1+K+K^2)+(m+1)N≤1+n(1+K+K2)+(m+1) and the corresponding dense matrix coefficient bound make the polynomial-size conclusion explicit.

What the exact representation provides

The equivalence retains every original policy coefficient and objective threshold. It therefore preserves the entire robust feasible epigraph, including instances with no feasible policy and optimization problems whose values are unbounded. The goal also states equality of attainable thresholds and preservation of minimizers for the same linear objective ttt in the finite SDP. It does not assume that either problem has a minimizer. Equality of a pair of real-valued infima would express less information and could conceal degenerate cases.

The mathematical results are established in the textbook. This mission supplies open Lean theorem statements for their formal verification and concrete definitions for their objects. The homogeneous S-lemma and the inhomogeneous S-procedure are already Proved on Prove2Me and are retained as references. The moment-hull identity and the complete quadratic-policy representation are the new targets. Their definition layer can also support work on polynomial policies and other lifted uncertainty sets.

Difficulty

Checking a quadratic constraint on an ellipsoid is a global requirement. Evaluating it at a finite collection of sample points does not establish the required universal inequality. Likewise, the image of a convex uncertainty set under the quadratic lift is generally not convex. The target must identify its whole convex hull, including compactness and boundary points.

The formalization must also preserve information restrictions through every matrix coefficient. Full observation cannot replace PjzP_jzPj​z, even if the resulting semidefinite program is easier to describe. The objective has uncertain affine data and participates in the same robust requirement as the constraints. These issues distinguish the complete statement from a single quadratic inequality or a result that assumes all coefficient columns are certain.

Formalization scope

All spaces and matrices are finite dimensional over the reals. The code uses finite functions for coordinates, but defines the uncertainty set through a sum of squares, so the norm is Euclidean. Matrix indices have a distinguished first coordinate. The unshifted lift has zero there; the positive-semidefinite moment block has one. Positive semidefiniteness also enforces symmetry of the moment matrix.

The model, uncertainty set, policy evaluation, original robust epigraph, and proposed SDP constraints are separate concrete definitions. Neither feasibility equivalence nor the moment-hull identity is assumed in the definitions. The theorem quantifies over every finite dimension, including zero; an empty observation list produces a constant policy. No division by a dimension or a policy-dependent denominator occurs.

The polynomial-size statement concerns the explicit real SDP representation, as in the book. It does not add a machine model or a bit-complexity theorem for an SDP solver. The formalization uses full quadratic coefficient arrays, so its stated counts need not be minimal. The bound includes all these redundant coefficients. There are no optional variants in this mission. The recorded sharpness observation about QQQ explains why its injectivity is retained in the compactness theorem.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI: 10.1515/9781400831050. Definition 14.3.1, printed p. 371; equation (14.3.6), printed p. 375; Lemma 14.3.7 and Corollary 14.3.8, printed pp. 384–385. The pinned PDF pages are respectively 397, 401, and 410–411.
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Robust Optimization XIV: Extreme-Scenario Reduction in Multistage InventoryTextbook

Inventory decisions under uncertain demand

An inventory manager chooses replenishment orders before knowing all future demand. Orders made today affect both the stock available tomorrow and the cost of later decisions. A flexible commitment contract adds another consideration: deviations from previously announced orders can incur penalties. The uncertainty therefore concerns a sequence of observations, and the object being optimized is a sequence of decision rules. Chapter 15 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization uses this setting to compare the cost of unrestricted adaptive policies with the cost of affine policies.

For such a comparison, an exact benchmark matters. Evaluating a policy against every trajectory in a continuous uncertainty set can require infinitely many constraints. The chapter's Lemma 15.2.1 identifies a class of problems whose optimal value is preserved by restricting uncertainty to finitely many extreme scenarios. This mission formalizes that general lemma, which the book applies to inventory management, rather than the numerical experiments or a particular contract data set.

A multistage convex model

A history at stage ttt is the tuple dt−1=(d0,…,dt−1)d^{t-1}=(d_0,\ldots,d_{t-1})dt−1=(d0​,…,dt−1​), where each observation djd_jdj​ is a real vector of dimension njn_jnj​. A policy specifies a real decision vector St(dt−1)S_t(d^{t-1})St​(dt−1) of dimension mtm_tmt​ for every possible history. Dependence only on observations already available is called nonanticipativity. Two full trajectories with identical observed prefixes necessarily produce the same decision at that stage.

There are T+1T+1T+1 decision stages and uncertainty sets F0,…,FTF_0,\ldots,F_TF0​,…,FT​. All data except the observations are fixed. Linear maps At,Bt+1,Ct+1A_t,B_{t+1},C_{t+1}At​,Bt+1​,Ct+1​ and vectors btb_tbt​ impose the initial and linking inequalities

A1S1(d0)≥b1,A_1S_1(d^0)\ge b_1,A1​S1​(d0)≥b1​, At+1St+1(dt)≥Bt+1dt+Ct+1St(dt−1)+bt+1,1≤t≤T.A_{t+1}S_{t+1}(d^t)\ge B_{t+1}d^t+C_{t+1}S_t(d^{t-1})+b_{t+1},\qquad 1\le t\le T.At+1​St+1​(dt)≥Bt+1​dt+Ct+1​St​(dt−1)+bt+1​,1≤t≤T.

Vector inequalities hold coordinatewise. The term Bt+1dtB_{t+1}d^tBt+1​dt uses the whole observed prefix. A fixed real bound RRR restricts the infinity norm of each decision at stages 1,…,T1,\ldots,T1,…,T. The terminal decision ST+1S_{T+1}ST+1​ still appears in the last linking constraint, but the printed norm restriction does not cover it.

Each decision incurs a stage cost ftf_tft​. The costs are lower semicontinuous convex functions with polyhedral effective domains. A cost may be +∞+\infty+∞ outside its domain; within the domain it is finite. Polyhedrality of the domain does not require the cost itself to be piecewise linear. The total cost includes all T+1T+1T+1 stages.

Formalization target

Write Opt⁡(F0,…,FT)\operatorname{Opt}(F_0,\ldots,F_T)Opt(F0​,…,FT​) for the infimum of all real bounds EEE for which some policy satisfies the preceding constraints and

∑t=1T+1ft(St(dt−1))≤Efor every dT∈F0×⋯×FT.\sum_{t=1}^{T+1}f_t(S_t(d^{t-1}))\le E \qquad\text{for every }d^T\in F_0\times\cdots\times F_T.t=1∑T+1​ft​(St​(dt−1))≤Efor every dT∈F0​×⋯×FT​.

For nonempty polytopes Dt⊂RntD_t\subset\mathbb R^{n_t}Dt​⊂Rnt​, the target is the complete value equality in Lemma 15.2.1, printed p. 430:

Opt⁡(D0,…,DT)=Opt⁡(Ext⁡D0,…,Ext⁡DT).\operatorname{Opt}(D_0,\ldots,D_T) =\operatorname{Opt}(\operatorname{Ext}D_0,\ldots,\operatorname{Ext}D_T).Opt(D0​,…,DT​)=Opt(ExtD0​,…,ExtDT​).

Here Ext⁡D\operatorname{Ext}DExtD denotes the set of extreme points of DDD. Both sides optimize over unrestricted nonanticipative policies. The target does not restrict those policies to affine rules, assert that every fixed policy has its worst cost at an extreme trajectory, or assert attainment of the optimum. The source states this lemma without a local numbered proof sequence, so the mission has one goal and its concrete model definitions, with no additional milestone chain.

What the result makes possible

For interval uncertainty, the extreme observations are interval endpoints. The book uses this consequence to replace a box of demand trajectories by a finite scenario set. It then describes a finite optimization problem whose decisions must agree whenever their available information agrees. These are exact comparisons of optimal values for the specified models, not estimates of sampling error. The number of scenarios can still grow exponentially with the horizon, as the chapter discusses on printed pp. 430–432 of the source.

The formalization makes the policy information pattern, terminal-stage treatment, and extended-value convention explicit. These details are useful beyond the inventory application because the lemma permits arbitrary compatible linear constraints and convex stage costs. The current artifacts state the known textbook result in Lean; a successful statement build is not a proof of the lemma. The reusable definitions are concrete and contain no unproved mathematical assertions.

Why the statement requires care

The uncertainty set is a product, but decisions at different stages are connected by constraints. A decision chosen for one trajectory cannot be chosen independently of another trajectory sharing the same history. Consequently, a statement about a single convex function on a polytope does not by itself express the multistage result. The target must retain the order of policy choice and universal quantification over trajectories, the complete cost sum, and the information available at each decision.

The final stage introduces a separate boundary issue: its cost and feasibility constraints remain present even though the printed bound stops one stage earlier. Omitting the final cost or extending the bound would change the problem. Degenerate and infeasible instances also require a value convention that does not assign them an arbitrary real number.

Formalization scope

Lean represents observations and decisions by finite real coordinate spaces, with dimensions allowed to vary by stage. Histories are finite dependent tuples; a policy's argument type contains exactly the observed prefix. Linear maps represent the book's matrices, including maps from stacked histories. Nonempty polytopes are convex hulls of nonempty finite sets, allowing singletons and lower-dimensional polytopes. The cost-domain predicate uses finitely many nonstrict matrix inequalities.

The extended optimal value is an EReal infimum of achievable real objective bounds. An empty set of bounds gives +∞+\infty+∞, while bounds unbounded below give −∞-\infty−∞. No subtraction of infinities occurs. Regular costs exclude −∞-\infty−∞, so the finite sum in the objective has no mixed-infinity ambiguity. The definition does not assume feasibility, boundedness below, or attainment. Zero horizon and zero-dimensional coordinate spaces follow the same displayed formulas.

Formalization Note No singleton assumption is placed on D0D_0D0​, and no measurability, continuity, or affine restriction is imposed on policies. The theorem expands its concrete model for independent auditing. A Lean type check verifies agreement with the separately named reusable definitions. The required mathematical infrastructure includes convex hulls, extreme points, lower semicontinuity, finite linear algebra, and extended-real order. Completion requires a proof of the stated value equality with precisely these hypotheses.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009, Chapter 15, §15.2.4.1, Lemma 15.2.1, printed p. 430 (PDF p. 456). DOI: 10.1515/9781400831050.
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Robust Optimization XI: Finite Reformulations of Worst-Case Convex LossTextbook

Robust fitting with uncertain measurements

Regression and classification fit a parameter vector to observed data. When measurements can vary within a prescribed set, a fit judged only at the nominal observations need not control its loss on the possible data. A worst-case loss constraint requires the loss bound to hold for every admissible matrix of measurements. Such a requirement can contain infinitely many inequalities even when the parameter vector has finitely many coordinates. Chapter 12 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization (2009) identifies structural assumptions under which this requirement has an exact finite convex representation.

This mission concerns the representation in Theorem 12.2.5. Its application is to robust fitting problems whose uncertainty support function separates into a feature-dependent factor and the infinity norm of a residual-space vector. The result applies to both symmetric losses, such as norms of regression residuals, and asymmetric losses formed from positive residual parts.

Data, residuals, and loss

Let n,ℓ,mn,\ell,mn,ℓ,m be positive integers. The nominal data matrix Zn∈Rn×mZ^n\in\mathbb R^{n\times m}Zn∈Rn×m has one column per measurement and one row per feature. For a parameter vector θ∈Rn\theta\in\mathbb R^nθ∈Rn, its residual vector is r=(Zn)Tθ∈Rmr=(Z^n)^T\theta\in\mathbb R^mr=(Zn)Tθ∈Rm. A fixed matrix U∈Rn×ℓU\in\mathbb R^{n\times\ell}U∈Rn×ℓ describes the structure of permitted perturbations, and a nonnegative scalar ρ\rhoρ controls their size. The uncertain data matrices are

Z={Zn+ρUΔ:Δ∈D},\mathcal Z=\{Z^n+\rho U\Delta:\Delta\in D\},Z={Zn+ρUΔ:Δ∈D},

where D⊂Rℓ×mD\subset\mathbb R^{\ell\times m}D⊂Rℓ×m is convex, compact, and contains zero. No independence of its columns is imposed.

The loss function L:Rm→RL:\mathbb R^m\to\mathbb RL:Rm→R is finite and convex. Assumption L requires one of two forms: L(r)=π(∣r∣)L(r)=\pi(|r|)L(r)=π(∣r∣) for every rrr, or L(r)=π(r+)L(r)=\pi(r_+)L(r)=π(r+​) for every rrr. Absolute value and positive part act coordinatewise. The function π\piπ is convex and nondecreasing in every coordinate on the nonnegative orthant. The choice of form is global, rather than chosen separately at each residual.

Assumption A specifies the support of DDD in every rank-one direction:

max⁡Δ∈DuTΔv=ϕ(u)ψ(v).\max_{\Delta\in D}u^T\Delta v=\phi(u)\psi(v).Δ∈Dmax​uTΔv=ϕ(u)ψ(v).

Here ϕ\phiϕ is finite, nonnegative, convex, and positively homogeneous, and ψ\psiψ is a norm. The goal uses ψ(v)=∥v∥∞\psi(v)=\|v\|_\inftyψ(v)=∥v∥∞​. These are the standing objects and assumptions of Section 12.2, printed pages 311–319 of the source.

Formalization targets

For any real threshold τ\tauτ, the goal is the exact equivalence

∀Z∈Z: L(ZTθ)≤τ\forall Z\in\mathcal Z:\ L(Z^T\theta)\le\tau∀Z∈Z: L(ZTθ)≤τ

if and only if there exists a real κ\kappaκ satisfying

ρϕ(UTθ)≤κ,L((Zn)Tθ+κei)≤τ,L((Zn)Tθ−κei)≤τ(1≤i≤m).\rho\phi(U^T\theta)\le\kappa,\qquad L((Z^n)^T\theta+\kappa e_i)\le\tau,\qquad L((Z^n)^T\theta-\kappa e_i)\le\tau\quad(1\le i\le m).ρϕ(UTθ)≤κ,L((Zn)Tθ+κei​)≤τ,L((Zn)Tθ−κei​)≤τ(1≤i≤m).

The goal also states convexity in (θ,κ)(\theta,\kappa)(θ,κ) of the scalar functions on the left of these constraints. There are 2m2m2m shifted-loss inequalities and one amplitude inequality.

The numbered supporting targets preserve the source's identities. Equation 12.2.11 gives the Fenchel biconjugate representation of a finite convex loss. Equation 12.2.12 equates the worst-case realized loss with its conjugate expression involving the support of DDD. Equation 12.2.15 replaces that support by its factorization under Assumption A. Equation 12.2.18 equates the resulting worst-case loss with a maximum over the dual unit ball:

Lwc(r,κ)=max⁡ψ∗(ξ)≤1L(r+κξ),κ≥0.L_{\rm wc}(r,\kappa)=\max_{\psi^*(\xi)\le1}L(r+\kappa\xi),\qquad \kappa\ge0.Lwc​(r,κ)=ψ∗(ξ)≤1max​L(r+κξ),κ≥0.

The maxima in these identities are required to be attained. The Fenchel representation itself uses the source's supremum notation.

What the representation provides

Theorem 12.2.5 replaces a constraint over a continuum of data matrices with finitely many evaluations of the original loss and the uncertainty gauge. It retains the dependence of uncertainty on the fitted parameter through ϕ(UTθ)\phi(U^T\theta)ϕ(UTθ). Consequently, the representation describes exactly the robust feasible parameters, including zero uncertainty, rather than merely giving a sufficient condition. Evaluation efficiency remains relative to the supplied loss and gauge, as in the book's tractability discussion.

The mathematical result is established in the textbook. The contribution sought here is a machine-checked formalization of its statement and supporting identities. The general finite-dimensional Fenchel biconjugacy theorem already has a proved platform item and is reused as the first milestone; the other three identities and the capstone are open theorem statements in this draft.

Mathematical difficulty

The central issue is relating uncertainty in a matrix to uncertainty in the residual vector while preserving exactness. A uniform bound on individual matrix entries does not by itself express Assumption A. Conjugate functions also need extended values: replacing an infinite conjugate by a real default would change the optimization problem. Establishing equality of optimal values alone is insufficient for identities written with maxima; their attainment is part of the targets. The zero-amplitude case must agree with the nominal loss throughout.

Formalization scope

Vectors use finite-dimensional real Euclidean spaces and matrices have explicitly ordered feature and measurement indices. Coordinates use Fin m, so the first coordinate is indexed by zero. The infinity norm in the goal is taken on the plain coordinate function; it is not the Euclidean norm of the residual vector. The statements include both signs for every coordinate.

The published fenchelConjugate and fenchelBiconjugate definitions are reused. Conjugate objectives take values in EReal. Every claimed maximum is expressed using IsGreatest at a common finite real value, so existence, boundedness, equality, and attainment remain visible. The inner support supremum in Equation 12.2.12 is real-valued and ranges over a nonempty compact image. The dual unit ball in Equation 12.2.18 is represented directly by ξTv≤ψ(v)\xi^Tv\le\psi(v)ξTv≤ψ(v) for all vvv.

All hypotheses about the loss, gauge, norm, and uncertainty set are explicit in each new theorem. None assumes the desired finite reformulation. Assumption L is retained despite the recorded observation that a weaker loss hypothesis suffices for the mathematical equivalence. There are no variant targets. A computational cost model and an optimization algorithm are outside this formalization; the explicit finite formulas and their convexity are the representation being formalized. Reusable work includes finite-dimensional conjugacy, compact support maximization, and dual-norm geometry.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI: 10.1515/9781400831050. Section 12.2, printed pp. 311–319; Equations 12.2.11, 12.2.12, 12.2.15, 12.2.18 and Theorem 12.2.5.
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Robust Optimization II: Safe Robust Counterparts for Bounded Random PerturbationsTextbook

Motivation: reliability under random data

A linear constraint can fail when its coefficients vary. In an engineering or planning model, requiring it to hold for every imaginable realization may exclude useful decisions, while checking it only at an average realization may give little control over failure. A chance constraint specifies an acceptable probability of violation. Chapter 2 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization studies deterministic convex conditions that guarantee this probabilistic requirement for a single uncertain linear inequality.

The chapter distinguishes a guarantee from an exact description of chance feasibility. Its robust constraints are safe approximations: satisfying them guarantees reliability, but a reliable decision need not satisfy them. The goal here concerns how known bounds on the perturbations can be incorporated into such an approximation without losing an explicit convex representation.

Setting: an uncertain scalar inequality

A decision is a vector x∈Rnx\in\mathbb R^nx∈Rn. The deterministic data are vectors a0,a1,…,aLa^0,a^1,\ldots,a^La0,a1,…,aL and scalars b0,b1,…,bLb^0,b^1,\ldots,b^Lb0,b1,…,bL. Define the residual coordinates by zi(x)=(ai)Tx−biz_i(x)=(a^i)^Tx-b^izi​(x)=(ai)Tx−bi, including the nominal coordinate i=0i=0i=0. A realized perturbation ζ∈RL\zeta\in\mathbb R^Lζ∈RL satisfies the constraint exactly when

z0(x)+∑i=1Lζizi(x)≤0.z_0(x)+\sum_{i=1}^L\zeta_i z_i(x)\le0.z0​(x)+i=1∑L​ζi​zi​(x)≤0.

For a probability law PPP and a tolerance 0<ε<10<\varepsilon<10<ε<1, chance feasibility means that the strict reverse inequality has probability at most ε\varepsilonε. Robust feasibility over a deterministic set ZZZ means that the displayed inequality holds for every η∈Z\eta\in Zη∈Z.

The perturbation coordinates are independent measurable real random variables. Their moment-generating functions obey the two-sided bound

EPetζi≤exp⁡(max⁡{μi−t,μi+t}+12σi2t2)(t∈R),\mathbb E_P e^{t\zeta_i}\le\exp\left(\max\{\mu_i^-t,\mu_i^+t\}+\frac12\sigma_i^2t^2\right)\qquad(t\in\mathbb R),EP​etζi​≤exp(max{μi−​t,μi+​t}+21​σi2​t2)(t∈R),

where μi−≤μi+\mu_i^-\le\mu_i^+μi−​≤μi+​ and σi≥0\sigma_i\ge0σi​≥0. These are the book's assumptions P.1–2. The goal additionally assumes almost-sure support bounds ai−≤ζi≤ai+a_i^-\le\zeta_i\le a_i^+ai−​≤ζi​≤ai+​, with finite endpoints satisfying ai−≤μi−≤μi+≤ai+a_i^-\le\mu_i^-\le\mu_i^+\le a_i^+ai−​≤μi−​≤μi+​≤ai+​. No positive lower bound on σi\sigma_iσi​ is imposed.

Formalization targets

Write B(y)=∑imax⁡{μi−yi,μi+yi}B(y)=\sum_i\max\{\mu_i^-y_i,\mu_i^+y_i\}B(y)=∑i​max{μi−​yi​,μi+​yi​}, D(y)=∑iσi2yi2D(y)=\sqrt{\sum_i\sigma_i^2y_i^2}D(y)=∑i​σi2​yi2​​, and rε=2log⁡(1/ε)r_\varepsilon=\sqrt{2\log(1/\varepsilon)}rε​=2log(1/ε)​. The general safety statement, Proposition 2.4.1, asserts that

z0+B(z)+rεD(z)≤0⟹P{z0+∑iziζi>0}≤ε.z_0+B(z)+r_\varepsilon D(z)\le0\quad\Longrightarrow\quad P\{z_0+\sum_i z_i\zeta_i>0\}\le\varepsilon.z0​+B(z)+rε​D(z)≤0⟹P{z0​+i∑​zi​ζi​>0}≤ε.

Its feasible set is convex. Proposition 2.4.2 states the tail bound at every nonnegative safety level rrr:

P{∑iziζi>B(z)+rD(z)}≤e−r2/2.P\{\sum_i z_i\zeta_i>B(z)+rD(z)\}\le e^{-r^2/2}.P{i∑​zi​ζi​>B(z)+rD(z)}≤e−r2/2.

Theorem 2.4.3 identifies the first deterministic inequality with robust feasibility over the moment uncertainty set

Zmom={η:∃w, μi−≤ηi−σiwi≤μi+ (1≤i≤L), ∑iwi2≤rε}.Z_{\rm mom}=\{\eta:\exists w,\ \mu_i^-\le\eta_i-\sigma_iw_i\le\mu_i^+\ (1\le i\le L),\ \sqrt{\sum_iw_i^2}\le r_\varepsilon\}.Zmom​={η:∃w, μi−​≤ηi​−σi​wi​≤μi+​ (1≤i≤L), i∑​wi2​​≤rε​}.

The capstone is Theorem 2.4.4. Let ZZZ be the intersection of ZmomZ_{\rm mom}Zmom​ with the support box [a−,a+][a^-,a^+][a−,a+]. Then xxx is robust feasible over ZZZ if and only if there exist extended residual vectors u,v∈RL+1u,v\in\mathbb R^{L+1}u,v∈RL+1 satisfying

zi(x)=ui+vi(0≤i≤L),z_i(x)=u_i+v_i\quad(0\le i\le L),zi​(x)=ui​+vi​(0≤i≤L), u0+∑imax⁡{ai−ui,ai+ui}≤0,v0+B(v)+rεD(v)≤0.u_0+\sum_i\max\{a_i^-u_i,a_i^+u_i\}\le0,\qquad v_0+B(v)+r_\varepsilon D(v)\le0.u0​+i∑​max{ai−​ui​,ai+​ui​}≤0,v0​+B(v)+rε​D(v)≤0.

This system is convex in its decision and auxiliary variables. Every feasible triple has violation probability at most ε\varepsilonε. The theorem includes both the deterministic equivalence and the probabilistic guarantee, as on printed page 48.

Two supporting targets retain the chapter's bounded mean-zero specialization. Proposition 2.3.1 gives the tail estimate P{∑iziζi>r∑izi2}≤e−r2/2P\{\sum_i z_i\zeta_i>r\sqrt{\sum_i z_i^2}\}\le e^{-r^2/2}P{∑i​zi​ζi​>r∑i​zi2​​}≤e−r2/2 for independent mean-zero perturbations in [−1,1][-1,1][−1,1]. Proposition 2.3.3 identifies robustness over the intersection of the unit box and a Euclidean ball with its lifted conic system and establishes the corresponding chance guarantee. These are supporting statements from the source, not replacements for the general capstone.

Significance: explicit conditions with a probability guarantee

The capstone connects a deterministic set of allowed perturbations with a stochastic model specified through moment bounds and support information. It gives a finite convex system whose feasible decisions satisfy the requested reliability level for every law meeting those assumptions. The statement does not require choosing a particular parametric distribution or estimating a probability separately for every decision.

These are known textbook results. The formalization targets are their Lean statements and eventual machine-checked proofs, including zero scales and boundary feasibility. The reusable content comprises finite-dimensional uncertainty sets, explicit exponential-moment hypotheses, and the relationship between lifted convex constraints and strict-event probabilities. The present authoring pass leaves the six theorem proofs open; compilation checks their types, not their truth.

Difficulty: boundary cases carry mathematical content

The exact robust representation includes equality cases in the endpoint order and permits degenerate ellipsoids. A formulation restricted to positive scales or strict interior intersections would omit cases of the stated theorem. The chance guarantee must also include the boundary of the explicit safe set; it cannot be replaced by a condition requiring an additional strict margin.

The printed proofs have local discrepancies recorded in the mission findings: the proof of Proposition 2.4.2 omits a sum and invokes an open-interval risk bound at its excluded endpoint when the safety level is zero, the first line of the goal's proof uses a different radius, and the limiting argument on page 50 asserts a zero limit that fails for strictly feasible residuals. These findings concern the proofs, not counterexamples to the theorem statements. The goal retains the printed constants and hypotheses.

Formalization scope

The namespace is RobustOpt2009.ScalarChance. Vectors use real-valued functions on Fin L; the nominal coordinate is a separate real component. All Euclidean lengths are explicit square roots of sums of squares, avoiding the default function-space sup norm. Probability is evaluated under a probability measure, and all random coordinates are measurable. The exponential-moment definition includes integrability, preventing nonintegrable Bochner integrals from supplying default zero values.

Scaled coordinates σiwi\sigma_iw_iσi​wi​ implement the book's zero-denominator convention: a zero scale forces zero displacement. Robust feasibility is a universal inequality, so no empty or unbounded real supremum is used. The exponential-certificate set, its topological closure, and the perturbation uncertainty set remain separate concrete objects. No definition assumes the desired equivalence or tail bound. Finite sums include the zero-dimensional case, where the statements reduce to their deterministic or empty-event versions.

Further work consists of proving the stated concentration, convexity, and exact representation claims using these definitions and Mathlib's probability and finite-dimensional analysis. No variants are posed in this chapter.

Selected references

  • Aharon Ben-Tal, Laurent El Ghaoui and Arkadi Nemirovski, Robust Optimization, Princeton University Press, 2009, Chapter 2, especially printed pp. 29–33 and 45–50. DOI: 10.1515/9781400831050. Published citation basis; PDF pages are printed pages plus 26.
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Robust Optimization IV: The Bernstein Uncertainty SetTextbook

Chance constraints and robust feasibility

An optimization model can require a linear inequality to hold with high probability when its coefficients are random. Such a chance constraint controls the probability of violation, but its feasible set need not be convex or easy to describe. A conservative convex approximation can make the requirement usable within a larger optimization model. Chapter 4 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization studies when such approximations also have a robust interpretation: the inequality must hold for every perturbation in a deterministic uncertainty set.

The target here is the chapter's Bernstein construction. It starts from information about the joint exponential moments of a random vector, rather than a fixed list of scenarios. Its conclusion identifies exactly the uncertainty set associated with the conservative approximation. Exactness concerns the relationship between that approximation and robust feasibility; the approximation is still only a sufficient condition for the original chance constraint.

Probability model and conjugate data

Let ζ\zetaζ have probability distribution PPP on RL\mathbb R^LRL. A coefficient vector is a pair z=(z0,w)z=(z_0,w)z=(z0​,w), where z0∈Rz_0\in\mathbb Rz0​∈R and w∈RLw\in\mathbb R^Lw∈RL. The requirement is

P{z0+⟨w,ζ⟩>0}≤ϵ,0<ϵ<1.P\{z_0+\langle w,\zeta\rangle>0\}\le\epsilon,\qquad 0<\epsilon<1.P{z0​+⟨w,ζ⟩>0}≤ϵ,0<ϵ<1.

The violation event is strict. Equality in the underlying linear inequality therefore counts as feasible. The parameter ϵ\epsilonϵ controls the permitted probability of failure.

A logarithmic moment-generating majorant is a finite convex function Φ:RL→R\Phi:\mathbb R^L\to\mathbb RΦ:RL→R satisfying Φ(0)=0\Phi(0)=0Φ(0)=0 and

log⁡EPexp⁡⟨w,ζ⟩≤Φ(w)for all w.\log\mathbb E_P\exp\langle w,\zeta\rangle\le\Phi(w)\quad\text{for all }w.logEP​exp⟨w,ζ⟩≤Φ(w)for all w.

These are Assumption Q.1. They concern the joint distribution; independence of the coordinates is not required. Assumption Q.2 provides an affine conjugate representation

Φ(w)=sup⁡u∈RM{⟨w,Au+a⟩−ϕ(u)},\Phi(w)=\sup_{u\in\mathbb R^M}\{\langle w,Au+a\rangle-\phi(u)\},Φ(w)=u∈RMsup​{⟨w,Au+a⟩−ϕ(u)},

where AAA is linear, a∈RLa\in\mathbb R^La∈RL, and ϕ:RM→R∪{+∞}\phi:\mathbb R^M\to\mathbb R\cup\{+\infty\}ϕ:RM→R∪{+∞} is convex and lower semicontinuous. Every real sublevel set of ϕ\phiϕ is bounded. Allowing +∞+\infty+∞ permits restrictions on the effective domain without changing the ambient space.

Formalization targets

The goal is Theorem 4.2.5, printed pp. 85–86 of the book. Define the coefficient sets independently by

Zϵo={(z0,w):∃α>0, αz0+Φ(αw)≤log⁡ϵ},Zϵ=cl⁡Zϵo.Z^o_\epsilon=\{(z_0,w):\exists\alpha>0,\ \alpha z_0+\Phi(\alpha w)\le\log\epsilon\},\qquad Z_\epsilon=\operatorname{cl}Z^o_\epsilon.Zϵo​={(z0​,w):∃α>0, αz0​+Φ(αw)≤logϵ},Zϵ​=clZϵo​.

Define the auxiliary sublevel set and its affine image by

Uϵ={u:ϕ(u)≤log⁡(1/ϵ)},Zϵ=AUϵ+a.U_\epsilon=\{u:\phi(u)\le\log(1/\epsilon)\},\qquad \mathcal Z_\epsilon=AU_\epsilon+a.Uϵ​={u:ϕ(u)≤log(1/ϵ)},Zϵ​=AUϵ​+a.

The theorem says that UϵU_\epsilonUϵ​ is nonempty, convex, and compact and that

(z0,w)∈Zϵ  ⟺  z0+⟨ζ,w⟩≤0for every ζ∈Zϵ.(z_0,w)\in Z_\epsilon\iff z_0+\langle\zeta,w\rangle\le0\quad\text{for every }\zeta\in\mathcal Z_\epsilon.(z0​,w)∈Zϵ​⟺z0​+⟨ζ,w⟩≤0for every ζ∈Zϵ​.

It also retains the displayed perspective characterization and its probabilistic consequence:

(z0,w)∈Zϵ  ⟺  inf⁡β>0[z0+βΦ(β−1w)+βlog⁡(1/ϵ)]≤0,(z_0,w)\in Z_\epsilon\iff\inf_{\beta>0}\left[z_0+\beta\Phi(\beta^{-1}w)+\beta\log(1/\epsilon)\right]\le0,(z0​,w)∈Zϵ​⟺β>0inf​[z0​+βΦ(β−1w)+βlog(1/ϵ)]≤0,

and this condition implies the original chance constraint.

Four source-numbered milestones accompany the goal. Lemma B.1.1 identifies the closure of a homogenized convex sublevel set with the zero sublevel set of its perspective infimum, including finiteness and convexity of that function. Proposition 4.2.2 characterizes the Bernstein approximation and asserts its normal safety. Proposition 4.2.3 gives bounded sublevel sets for an affine conjugate representation whose linear map has trivial kernel. Theorem B.1.2 gives the general robust representation under its directional-limit assumption. Each statement retains its source hypotheses and all conclusion clauses.

Mathematical and formal significance

The chapter's result gives a deterministic meaning to a probabilistic sufficient condition. An uncertainty set chosen through the conjugate data describes precisely the same coefficient constraints as the Bernstein approximation. This connects the probability model to robust linear feasibility while preserving the distinction between a guarantee and an exact description of the original chance-feasible set.

The formalization supplies separate, concrete definitions for the probability condition, the coefficient cone, and the perturbation set. That separation makes the equality in the main result a substantive theorem. The appendix statements also expose reusable finite-dimensional convex analysis, including perspective values, closed cones, and affine images of extended-real sublevel sets. These are known mathematical results from the book; the current draft consists of type-checked statements awaiting Lean proofs. A successful statement build is not a proof of any of these assertions.

Difficulty

Closure and optimization at a boundary are central issues. The perspective infimum ranges over strictly positive scales, but its value may be approached only as the scale tends to zero. Replacing the infimum condition by the existence of one feasible scale would change the target. Similarly, an extended-real function can impose a proper effective domain, so a formalization restricted to everywhere-finite penalties would omit cases covered by the theorem.

The general appendix theorem includes a directional limit below a specified level. That limit can be negative infinity, including in the application to the chapter's coefficient variable. Requiring a finite real limit would exclude the intended application. Probability expressions also require attention to the strict violation event and to the meaning of an expectation when exponential moments diverge.

Formalization scope

Finite-dimensional real spaces are represented by functions on Fin n, with the standard topology. Coefficients are pairs (z0,w)(z_0,w)(z0​,w), so coefficient feasibility and perturbation membership have different types. The linear map is explicit and its affine translation is applied before taking the pairing. No independence, Gaussian distribution, bounded support, or injectivity assumption is added to the goal. Injectivity belongs only to Proposition 4.2.3 and its variant.

Formalization Note Infima and suprema are computed in the complete extended-real lattice. The penalty's negative-infinity value is explicitly excluded where the source uses R∪{+∞}\mathbb R\cup\{+\infty\}R∪{+∞}. Convexity is expressed by the real epigraph and lower semicontinuity by closed real sublevels. Q.1 uses the equivalent bound on the nonnegative integral of the exponential, avoiding a default real-integral value on nonintegrable inputs. The uncertainty set is the actual affine image of the specified sublevel set, not an assumed certificate for robust feasibility.

Beyond the paper. One additional target strengthens Proposition 4.2.3 by removing only lower semicontinuity. Finding F1 records that finite bounds in the positive and negative coordinate directions, together with injectivity, already bound each sublevel set. The faithful proposition retains lower semicontinuity and remains the milestone. This strengthening does not change the goal or remove the topological assumptions needed for compactness elsewhere.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI: 10.1515/9781400831050. Chapter 4, §§4.1–4.2.3, printed pp. 81–86 (PDF pp. 107–112); Appendix B, §§B.1.1–B.1.3, printed pp. 471–475 (PDF pp. 497–501). Citation basis: published.
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Robust Optimization III: Global Sensitivity for Linear ConstraintsTextbook

Motivation: controlling violations beyond normal uncertainty

A resource constraint can remain useful even when an exceptional disturbance makes exact satisfaction impractical. In such cases the model needs to distinguish the disturbances against which feasibility is mandatory from those for which a controlled violation is acceptable. Ordinary robust optimization specifies a set of perturbations and requires the constraint to hold everywhere in that set. It does not itself describe what happens outside that set. Chapter 3 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization introduces a quantitative way to make this distinction for uncertain linear inequalities.

The object of this mission is the globalized robust counterpart of a single scalar inequality. Its tolerance is proportional to distance from a normal uncertainty range, with a prescribed restriction on admissible displacement directions. The goal is Proposition 3.2.1, which characterizes this global requirement by two ordinary robust inequalities. The result is a known theorem of the book; the target here is its faithful Lean formalization.

Setting: a perturbation structure and a scalar constraint

Let x∈Rnx\in\mathbb R^nx∈Rn be a decision vector. The data consist of vectors a0,a1,…,aL∈Rna^0,a^1,\ldots,a^L\in\mathbb R^na0,a1,…,aL∈Rn and scalars b0,b1,…,bL∈Rb^0,b^1,\ldots,b^L\in\mathbb Rb0,b1,…,bL∈R. A perturbation vector ζ∈RL\zeta\in\mathbb R^Lζ∈RL determines the inequality

[a0+∑ℓ=1Lζℓaℓ]Tx≤b0+∑ℓ=1Lζℓbℓ.\left[a^0+\sum_{\ell=1}^L\zeta_\ell a^\ell\right]^Tx \le b^0+\sum_{\ell=1}^L\zeta_\ell b^\ell.[a0+ℓ=1∑L​ζℓ​aℓ]Tx≤b0+ℓ=1∑L​ζℓ​bℓ.

The normal range ZZZ is a nonempty closed convex subset of RL\mathbb R^LRL. A closed convex cone KKK containing zero describes the possible directions of departure. The physically possible range is the sum

Z+K={z+d:z∈Z, d∈K}.Z+K=\{z+d:z\in Z,\ d\in K\}.Z+K={z+d:z∈Z, d∈K}.

Here KKK denotes the book's L\mathcal LL; LLL remains the number of perturbation coordinates. A fixed norm NNN measures displacement. These are the perturbation-structure assumptions (G.a–c) on printed page 68 of the source.

For a physically possible perturbation, its constrained distance from the normal range is

d(ζ,Z∣K)=inf⁡{N(ζ−z):z∈Z, ζ−z∈K}.d(\zeta,Z\mid K)=\inf\{N(\zeta-z):z\in Z,\ \zeta-z\in K\}.d(ζ,Z∣K)=inf{N(ζ−z):z∈Z, ζ−z∈K}.

The displacement restriction is part of the definition. The admissible set of displacement lengths is nonempty when ζ∈Z+K\zeta\in Z+Kζ∈Z+K and is bounded below by zero. Thus the distance has a finite real value on precisely the domain where the counterpart uses it.

A nonnegative real parameter α\alphaα is the global sensitivity. Global robustness requires the residual of the uncertain inequality to be at most αd(ζ,Z∣K)\alpha d(\zeta,Z\mid K)αd(ζ,Z∣K) for every physically possible perturbation. This is Definition 3.1.1 and equation (3.1.4) of the book.

Formalization targets

Write the residual and its directional part as

rx(ζ)=[a0+∑ℓζℓaℓ]Tx−b0−∑ℓζℓbℓ,qx(d)=[∑ℓdℓaℓ]Tx−∑ℓdℓbℓ.r_x(\zeta)=\left[a^0+\sum_\ell\zeta_\ell a^\ell\right]^Tx-b^0-\sum_\ell\zeta_\ell b^\ell, \qquad q_x(d)=\left[\sum_\ell d_\ell a^\ell\right]^Tx-\sum_\ell d_\ell b^\ell.rx​(ζ)=[a0+ℓ∑​ζℓ​aℓ]Tx−b0−ℓ∑​ζℓ​bℓ,qx​(d)=[ℓ∑​dℓ​aℓ]Tx−ℓ∑​dℓ​bℓ.

The goal is the complete equivalence of Proposition 3.2.1, printed page 69:

[∀ζ∈Z+K, rx(ζ)≤αd(ζ,Z∣K)]⟺{rx(ζ)≤0∀ζ∈Z,qx(d)≤α∀d∈K with N(d)≤1.\bigl[\forall\zeta\in Z+K,\ r_x(\zeta)\le\alpha d(\zeta,Z\mid K)\bigr] \quad\Longleftrightarrow\quad \begin{cases} r_x(\zeta)\le0&\forall\zeta\in Z,\\ q_x(d)\le\alpha&\forall d\in K\text{ with }N(d)\le1. \end{cases}[∀ζ∈Z+K, rx​(ζ)≤αd(ζ,Z∣K)]⟺{rx​(ζ)≤0qx​(d)≤α​∀ζ∈Z,∀d∈K with N(d)≤1.​

Both right-hand requirements are universal inequalities. The nominal coefficients occur in the first and do not occur in the second. The directional condition includes the zero direction and every direction on the boundary of the unit ball.

There are no separate supporting theorem milestones in this mission. The numbered Chapter 1 representation results discussed after the proposition describe applications of its conclusion. They are not intermediate targets needed to state this capstone.

Significance: separating two kinds of robustness

The equivalence distinguishes feasibility throughout the normal range from control of how the residual varies along admissible directions. As explained in Remark 3.2.2 of the book, it brings the globalized counterpart into contact with representation results for ordinary robust constraints. The proposition itself remains valid without a boundedness assumption on the normal range and without choosing a special shape such as a box or ellipsoid.

The formalization fixes the exact relationship between the domain of the distance and the quantifiers in the counterpart. It also makes the treatment of the cone and the norm explicit. These conventions are useful when subsequent developments specialize the model. The mission asks for a proof of the displayed equivalence; finite reformulations for particular uncertainty geometries and the chapter's antenna-array application are outside this target.

Difficulty: distance domains and boundary cases

The constrained distance cannot generally be replaced by ordinary distance to ZZZ. That substitution changes which normal points are eligible when evaluating a disturbance. The normal range can also be unbounded, so compactness of ZZZ is not available as a standing assumption. A formal proof must handle the domain of the infimum and the full directional quantification with these features intact.

The parameter α\alphaα may be zero. In that case the globalized condition requires exact feasibility throughout Z+KZ+KZ+K, as noted after Definition 3.1.1 in the source. The cone may consist only of zero, and the relevant displacement can have zero norm. None of these cases is excluded by a positivity assumption added for convenience.

Formalization scope

All coefficients and sensitivities are real. Decision and perturbation vectors use the finite coordinate types Fin n and Fin L; their zero-based indexing is a relabeling of the source sums. The nominal coefficients are separate parameters. The goal writes the coordinate sums and constrained infimum explicitly, using only Mathlib objects, so its meaning does not depend on an unpublished definition from another chapter.

An arbitrary norm is represented by Mathlib's real seminorm type together with definiteness: N(v)=0N(v)=0N(v)=0 implies v=0v=0v=0. Closedness uses the usual topology on finite-dimensional real coordinate space. Convexity of both sets, nonemptiness of ZZZ, membership of zero in KKK, and closure of KKK under nonnegative scaling are explicit hypotheses. The global robustness condition is the distance inequality itself, not a definition chosen to assume its desired characterization.

The real infimum is used only over a nonempty set of nonnegative lengths. Its value on an empty set is not used by the theorem. Zero coordinate dimensions are permitted with empty sums interpreted as zero. The faithful goal retains convexity of ZZZ; the separately recorded observation that it is unnecessary does not alter this statement. The remaining formal work concerns this exact equivalence, using finite sums, convex sets, seminorms, topology and real infima from Mathlib.

Selected references

  • Aharon Ben-Tal, Laurent El Ghaoui and Arkadi Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI: 10.1515/9781400831050. Chapter 3, Definition 3.1.1 and equations (3.1.2)–(3.1.4), printed page 68 (PDF page 94); Proposition 3.2.1 and Remark 3.2.2, printed page 69 (PDF page 95); proof continuation, printed page 70 (PDF page 96).
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C*-Algebras and Direct Integral Decomposition for Lie Supergroups: Unitary Representations of a Lie Supergroup and Nondegenerate -Representations of Its C-Algebra Form Isomorphic CategoriesResearch Paper

Motivation

Unitary representations turn symmetries into operators on Hilbert spaces. For ordinary locally compact groups, the associated group C∗C^*C∗-algebra lets one study these operators through a single algebraic object. A Lie supergroup adds odd infinitesimal symmetries to an ordinary Lie group. Its unitary representations must respect both the group action and those odd operators. Neeb and Salmasian construct a C∗C^*C∗-algebra A(G,g)\mathcal A(G,\mathfrak g)A(G,g) that captures this combined structure Neeb–Salmasian 2015. The representation correspondence is the point at which their construction becomes useful: a representation of A\mathcal AA retains precisely the data of a unitary supergroup representation.

The paper subsequently uses this bridge to discuss direct integral decompositions through the C∗C^*C∗-algebra. This mission concerns the bridge itself, Theorem 6.4. Its input is not a special connected or nilpotent group: the paper works with an arbitrary finite-dimensional Lie supergroup. The later CCR results in §7 add hypotheses and are outside this mission.

Setting

A finite-dimensional Lie supergroup is a pair (G,g)(G,\mathfrak g)(G,g). Here GGG is a real Lie group and g=g0ˉ⊕g1ˉ\mathfrak g=\mathfrak g_{\bar 0}\oplus\mathfrak g_{\bar 1}g=g0ˉ​⊕g1ˉ​ is a real Lie superalgebra. Its even part g0ˉ\mathfrak g_{\bar 0}g0ˉ​ is the Lie algebra of GGG. The group acts smoothly on the superalgebra by an adjoint action whose even restriction is the derivative of conjugation; differentiation of the action recovers the superbracket. These are the conditions of Definition 2.1, including the finite-dimensional convention stated just after it.

A unitary representation consists of a graded complex Hilbert space H=H0ˉ⊕H1ˉ\mathcal H=\mathcal H_{\bar 0}\oplus\mathcal H_{\bar 1}H=H0ˉ​⊕H1ˉ​, a strongly continuous unitary action π\piπ of GGG preserving that grading, and a real-linear superalgebra action ρπ\rho^\piρπ on the space H∞\mathcal H^\inftyH∞ of smooth orbit vectors. On even elements, ρπ\rho^\piρπ equals the derived group action. On odd elements, e−πi/4ρπ(x)e^{-\pi i/4}\rho^\pi(x)e−πi/4ρπ(x) is symmetric, and the odd action transforms under GGG through the adjoint action. This is Definition 2.3, including its parity and bracket requirements.

The paper adjoins a parity element ε\varepsilonε and writes Gε=G×{1,ε}G_\varepsilon=G\times\{1,\varepsilon\}Gε​=G×{1,ε}. A test function on this group is a pair of smooth, compactly supported complex functions on GGG. Using the complex universal enveloping algebra, the authors form an algebraic crossed product A∘\mathcal A^\circA∘. A word D=x1⋯xkD=x_1\cdots x_kD=x1​⋯xk​ and a test function fff act in each unitary representation by the bounded operator ρπ(D)π(f)\rho^\pi(D)\pi(f)ρπ(D)π(f). The norm of an algebraic element is the supremum of the norms of these represented operators; completion after quotienting its zero seminorm gives the non-unital C∗C^*C∗-algebra A=A(G,g)\mathcal A=\mathcal A(G,\mathfrak g)A=A(G,g) §§3–4.

A star representation of A\mathcal AA on H\mathcal HH is nondegenerate when the span of its image applied to H\mathcal HH is dense. A morphism between two unitary supergroup representations is a bounded, even, complex-linear operator intertwining both their GGG-actions and their g\mathfrak gg-actions on smooth vectors. A morphism between C∗C^*C∗-algebra representations intertwines every element of A\mathcal AA.

Formalization targets

Uniform control and smooth multiplier action

The first targets are the uniform bound of Proposition 3.2 and the smoothness statement of Proposition 5.1. For each word DDD and test pair fff, the same constant works for every unitary representation:

∃MD,f>0∀(π,ρπ,H),∥ρπ(D)π(f)∥≤MD,f.\exists M_{D,f}>0\quad\forall(\pi,\rho^\pi,\mathcal H),\qquad \|\rho^\pi(D)\pi(f)\|\le M_{D,f}.∃MD,f​>0∀(π,ρπ,H),∥ρπ(D)π(f)∥≤MD,f​.

The left multiplier orbit g↦ηG(g)ag\mapsto\eta_G(g)ag↦ηG​(g)a is smooth for every a∈A∘a\in\mathcal A^\circa∈A∘. The construction from a nondegenerate representation also identifies its smooth vectors with the represented algebraic core, as in Lemma 6.2. These are the analytic steps named in the milestone list.

Isomorphism of representation categories

The goal is Theorem 6.4. Propositions 6.1 and 6.3 give mutually inverse assignments on objects, and Theorem 6.4 retains the same intertwiners:

URep⁡(G,g)  ≅  Rep⁡nd(A(G,g)).\operatorname{URep}(G,\mathfrak g) \;\cong\; \operatorname{Rep}_{\mathrm{nd}}\bigl(\mathcal A(G,\mathfrak g)\bigr).URep(G,g)≅Repnd​(A(G,g)).

Thus each unitary representation yields exactly one nondegenerate representation agreeing on every generator, each nondegenerate representation comes from exactly one unitary supergroup representation, and a bounded operator intertwines one pair exactly when it intertwines the other. The goal includes all three clauses.

Significance

The result lets questions about unitary Lie supergroup representations be transferred to a C∗C^*C∗-algebra without losing the odd infinitesimal action or the morphisms. In the paper, this is the foundation for the later direct integral discussion and CCR criteria. Without the equivalence, properties of A\mathcal AA would have no stated connection to decomposition of unitary supergroup representations §7.

The mathematical result is proved in the cited paper; the local Lean declarations are open statements. A complete formal development would add machine-checked proofs for the uniform operator bounds, the algebra and multiplier facts, reconstruction of the odd action, and the categorical equivalence. The reusable parts include smooth-vector actions, integrated test-function operators, and a universal bounded family of representations.

Difficulty

The odd infinitesimal operators are defined on H∞\mathcal H^\inftyH∞, not automatically as bounded operators on all of H\mathcal HH. Integrating π\piπ against a test function supplies smooth vectors, but it does not by itself give a bound for an arbitrary word in the odd and even operators that is uniform over every representation. That uniformity is needed to construct one C∗C^*C∗-norm. In the reverse direction, a nondegenerate representation of A\mathcal AA first gives bounded operators; recovering the derived action on precisely the smooth core requires the multiplier and smoothness statements. An object-level bijection alone would still miss the paper's assertion about intertwiners.

Formalization scope

Lean models GGG as a finite-dimensional smooth real Lie group, with g0ˉ\mathfrak g_{\bar 0}g0ˉ​ its Mathlib group Lie algebra and g1ˉ\mathfrak g_{\bar 1}g1ˉ​ a finite-dimensional real normed space. The superbracket and odd adjoint action are fields of a Harish–Chandra pair. Smoothness uses C∞C^\inftyC∞, not analyticity. The group is neither assumed connected nor second countable. A left Haar measure is fixed. The Hilbert spaces quantified in the mission belong to Type; the index of all such unitary representations belongs to Type 1.

The test space D(Gε)\mathcal D(G_\varepsilon)D(Gε​) is encoded as pairs of functions, and the enveloping-algebra elements needed here as finite words. A\mathcal AA is the closed non-unital star subalgebra of the bounded product of operator algebras generated by their representation families. This uses all Type-small unitary representations; the paper takes unitary-equivalence classes of cyclic ones, which yield the same norm through its Remark 2.5. The algebra depends only on (G,g)(G,\mathfrak g)(G,g) and Haar measure, and ρπ\rho^\piρπ acts on H∞\mathcal H^\inftyH∞ itself. This rules out a choice of algebra or an off-domain operator value that would make the correspondence automatic.

The published smooth-orbit and vector-integral definitions from van Dijk–Neeb–Salmasian–Zellner are reused. Completing this mission calls for the Dixmier–Malliavin factorization, Gårding smoothing, bounded operator estimates, non-unital C∗C^*C∗-algebra representations and multiplier actions. Contributions proving those general tools or the source-labelled milestones are within scope. The generator family is represented through vectors rather than an operator-norm Bochner integral, whose measurability is unavailable for a merely strongly continuous representation.

Selected references

  • K.-H. Neeb and H. Salmasian, “C*-algebras and direct integral decomposition for Lie supergroups,” arXiv:1506.01558v1, 2015. Preprint.
  • G. van Dijk, K.-H. Neeb, H. Salmasian and C. Zellner, On the characterization of trace class representations and Schwartz operators, arXiv:1512.02451v1, 2015. Preprint.
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Functional AnalysisQuantum Information·Captain: mikedeng1

Approximation of Multipartite Quantum States and the Relative Entropy of Entanglement: Lower Semicontinuity of the Relative Entropy of Entanglement at States with n−1 FA-Property MarginalsResearch Paper

Motivation

The relative entropy of entanglement measures how distinguishable a multipartite quantum state is from all fully separable states. In finite dimensions it is a standard entanglement measure, but infinite-dimensional systems raise a basic analytical problem: the measure may take the value +∞+\infty+∞, and finite-rank approximations do not automatically control its behavior at a limit state. Shirokov's analysis identifies a broad class of states at which the direct relative entropy of entanglement is finite and lower semicontinuous. The result applies when all but possibly one marginal state satisfy the FA-property, a spectral condition that includes useful finite-entropy states without requiring finite-dimensional Hilbert spaces.

The paper relates the direct measure to a universal extension formed from local finite-rank compressions. This mission isolates the ERE_RER​ part of Theorem 2 A) and the source results needed to reach it. A later paper by Lami and Shirokov addresses more general global lower semicontinuity questions using a different operator model and hypotheses; its statements are related work, not imports into this mission. Shirokov, §4.3; Lami–Shirokov.

Setting

There are nnn parties A1,…,AnA_1,\ldots,A_nA1​,…,An​, with separable Hilbert spaces HAs\mathcal H_{A_s}HAs​​. A state ρ\rhoρ is a positive trace-class operator with trace one on their joint system. Its marginal ρAs\rho_{A_s}ρAs​​ is obtained by tracing out every party except AsA_sAs​. A product state is a tensor product of one state per party. The set Ss\mathfrak S_sSs​ of fully separable states is the trace-norm closed convex hull of product states. Closure matters in infinite dimension: restricting to finite convex combinations would change the infimum below. Shirokov, pp. 10–11, (26).

Write H(ρ∥σ)H(\rho\|\sigma)H(ρ∥σ) for Lindblad's quantum relative entropy, including the trace correction for unnormalized positive operators and the value +∞+\infty+∞ on support failure. The direct relative entropy of entanglement is

ER(ρ)=inf⁡σ∈SsH(ρ∥σ).E_R(\rho)=\inf_{\sigma\in\mathfrak S_s}H(\rho\|\sigma).ER​(ρ)=σ∈Ss​inf​H(ρ∥σ).

The von Neumann entropy H(ρ)H(\rho)H(ρ) and ER(ρ)E_R(\rho)ER​(ρ) are extended nonnegative real quantities in natural-logarithm units. A state has the FA-property when its eigenvalues λj\lambda_jλj​ admit nonnegative numbers gjg_jgj​ with ∑jλjgj<+∞\sum_j\lambda_jg_j<+\infty∑j​λj​gj​<+∞ and lim⁡β↓0(∑je−βgj)β=1\lim_{\beta\downarrow0}(\sum_je^{-\beta g_j})^\beta=1limβ↓0​(∑j​e−βgj​)β=1. In particular, the FA-property implies finite entropy. The set S∗\mathfrak S_*S∗​ consists of joint states with the FA-property on at least n−1n-1n−1 marginals. Shirokov, pp. 2, 4, 14, (1), (34).

For each party, a finite-rank orthogonal projector compresses the joint state. The universal extension E^R\widehat E_RER​ takes the supremum of the homogeneous ERE_RER​ values of all such local compressions. A compressed positive operator XXX with trace c>0c>0c>0 is valued as cER(X/c)cE_R(X/c)cER​(X/c); the zero operator has value zero. Local spectral projectors built from the marginals define the approximation ΛrL(ρ)\Lambda_r^L(\rho)ΛrL​(ρ) used in Theorem 1. Shirokov, pp. 7, 12–13, (17), (31).

Formalization targets

Goal: Theorem 2 A), the ERE_RER​ case

For ρ0∈S∗\rho_0\in\mathfrak S_*ρ0​∈S∗​, ER(ρ0)<+∞E_R(\rho_0)<+\inftyER​(ρ0​)<+∞. For every sequence of states ρk→ρ0\rho_k\to\rho_0ρk​→ρ0​ in trace norm,

ER(ρ0)≤lim inf⁡k→∞ER(ρk).E_R(\rho_0)\le\liminf_{k\to\infty}E_R(\rho_k).ER​(ρ0​)≤k→∞liminf​ER​(ρk​).

The sequence itself may lie anywhere in the full state space. This is the sequential lower semicontinuity assertion (35), together with finiteness, in Theorem 2 A).

Supporting targets

The milestones, in attack order, are: the FA entropy consequence (p. 4); the pure-state separable comparison of Lemma 3; the σ\sigmaσ-convexity of ERE_RER​ (first sentence of Theorem 2 E)); the upper bound (28) by any n−1n-1n−1 marginal entropies,

ER(ρ)≤∑s≠tH(ρAs);E_R(\rho)\le\sum_{s\ne t}H(\rho_{A_s});ER​(ρ)≤s=t∑​H(ρAs​​);

the concavity-defect bound (27), pER(ρ)+(1−p)ER(σ)≤ER(pρ+(1−p)σ)+h2(p)pE_R(\rho)+(1-p)E_R(\sigma)\le E_R(p\rho+(1-p)\sigma)+h_2(p)pER​(ρ)+(1−p)ER​(σ)≤ER​(pρ+(1−p)σ)+h2​(p); membership of ERE_RER​ in Lnn−1(1,1)L_n^{n-1}(1,1)Lnn−1​(1,1); the LLL-class assertion of Theorem 1; the relative-entropy inequality of Lemma 1 for positive maps with trace-preserving sum; the comparison E^R≤ER\widehat E_R\le E_RER​≤ER​; lower semicontinuity of E^R\widehat E_RER​; and the equality ER=E^RE_R=\widehat E_RER​=ER​ on S∗\mathfrak S_*S∗​ (Theorem 2 B)). These are claims made in the paper, with the portions outside the ERE_RER​ route explicitly scoped in the item descriptions. Shirokov, pp. 4, 8, 11, 13–15, 20, 25.

Significance

The theorem gives a stable finite value of ERE_RER​ at every state in S∗\mathfrak S_*S∗​: approximating sequences cannot converge there while hiding a smaller limiting value. This matters when infinite-dimensional states are approximated by finite-rank or energy-constrained states, because pointwise convergence of operators alone does not control an extended-valued entanglement measure. The equality with E^R\widehat E_RER​ also identifies the direct measure with a globally lower semicontinuous construction on the stated domain. Shirokov, Theorem 2 and discussion in §4.3.

The mathematical result is proved in the source paper. The formalization work is to express its spectral FA condition, multipartite partial traces, trace-norm separability, finite-rank compression, homogeneous extension, and extended-real inequalities in Lean, then prove the milestones and goal. The published P01 definition already supplies von Neumann entropy and Lindblad relative entropy; the propositions in this mission are open Lean statements, not machine-checked proofs. This shared infrastructure can support other infinite-dimensional quantum information results involving separability and marginal entropies.

Difficulty

A direct argument from the infimum defining ERE_RER​ cannot simply exchange that infimum with a state limit: the separable comparison state that nearly minimizes at one point need not remain useful along a convergent sequence. Infinite values also make real-valued continuity bounds insufficient. The paper's theorem therefore has to coordinate a finite-entropy estimate on n−1n-1n−1 marginals with control of local finite-rank approximations and a lower semicontinuous extension. The approximation estimate is uniform over a class of functions, with the rank threshold and error sequence chosen before the function. Shirokov, Theorem 1 and proof of Theorem 2 A).

Formalization scope

Each HAs\mathcal H_{A_s}HAs​​ is represented as ℓ2(Is)\ell^2(I_s)ℓ2(Is​) for a countable basis index type. Parties are indexed by Fin⁡(n)\operatorname{Fin}(n)Fin(n), and the joint basis uses their dependent Cartesian product. The state topology is the trace-norm topology of the published P33 state structure. Entropy, relative entropy, and ERE_RER​ take values in [0,+∞][0,+\infty][0,+∞]; no real-valued surrogate replaces an infinite value. The FA-property requires an actual orthonormal eigenbasis tied to the state's coefficients. Its partition sum is computed in [0,+∞][0,+\infty][0,+∞], so divergence cannot default to zero. The definition of S∗\mathfrak S_*S∗​ says at least n−1n-1n−1 FA marginals and does not impose FA on the sequence in the goal.

The Lnm(C,D)L_n^m(C,D)Lnm​(C,D) class is represented with a finite set of FA parties in place of the first mmm parties, reflecting the paper's relabeling symmetry. Within that class, ERE_RER​ is converted to a real number only on the finite-entropy domain. The universal extension uses all finite orthonormal local families and the homogeneous convention for compressed positive operators. The setting also defines countable separable decompositions, finite-rank projectors, the spectral approximation relation, binary entropy in nats, and positive linear maps on the trace class. The proviso of (27) that "all the involved quantities are finite" (p. 11) is stated as finiteness of ERE_RER​ at the two mixed states. These definitions and the cited P01/P33 libraries are the reusable work. A definition of FA that every state satisfies, a separable set without trace closure, or a real ERE_RER​ that discards +∞+\infty+∞ would trivialize or alter the target.

The paper also states a regularized ER∞E_R^\inftyER∞​ case. It is outside this mission: its proof in version 2 invokes propositions by broken “??” references that are absent from the source. The hatted-class and NNN-class portions of Theorem 1, the regularized equality in Theorem 2 B), and the entanglement-monotone part of the universal-extension bullet are likewise outside these ERE_RER​ milestones. Contributions proving the stated Lean milestones, improving the common operator definitions, and then proving the goal are welcome.

Selected references

  • M. E. Shirokov, Approximation of multipartite quantum states and the relative entropy of entanglement, arXiv preprint, version 2, 2024. arXiv:2103.12111v2.
  • L. Lami and M. E. Shirokov, Attainability and lower semi-continuity of the relative entropy of entanglement, and variations on the theme, arXiv preprint, 2021. arXiv:2105.08091.
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EconomicsOperations Research·Captain: mikedeng1

Managing Capital Market Frictions via Cost-Reduction Investments: A Positive Friction Effect Makes Cost-Reduction Investment More Beneficial Under Capital Market Frictions than in Their AbsenceResearch Paper

Why financing changes a production investment

A firm that can lower its unit production cost must usually spend money before it sells anything. That payment improves the margin on future sales but leaves less cash to fund production. If the firm borrows the shortfall, the investment can therefore change both its operating return and the cost of financing. Tanrisever, Joglekar, Erzurumlu and Lévesque (2021) study this tension in a two-stage model of a capital-constrained producer facing uncertain demand. Their Proposition 4 asks when the producer gains more from the investment in a market with bankruptcy costs than in a frictionless capital market.

The question matters for a production decision made before demand is known. A cost reduction may permit a larger production quantity and increase the return on each sale. It may also reduce the size and risk of the required loan, although paying for the investment consumes capital first. The paper isolates these effects so that the sign of the financing contribution can be examined separately from the direct operating gain. This mission covers that analytic comparison in §3 of the published paper, not its later numerical experiments or uncertain-investment extension.

Firm, demand, and competitive loan

The firm sells each unit for p>0p>0p>0. It chooses a nonnegative production quantity qqq before demand ξ\xiξ is realized; demand is uniform on [0,a][0,a][0,a] with a>0a>0a>0. Revenue is pmin⁡(q,ξ)p\min(q,\xi)pmin(q,ξ). The firm starts with unit production cost c1>0c_1>0c1​>0 and capital y1y_1y1​. It may invest A>0A>0A>0 to reduce unit cost by βA\beta AβA, where β>0\beta>0β>0 is cost reduction per dollar. Its post-investment cost and capital are c2=c1−βA>0c_2=c_1-\beta A>0c2​=c1​−βA>0 and y2=y1−A≥0y_2=y_1-A\ge0y2​=y1​−A≥0. Without investment, the corresponding pair remains (c1,y1)(c_1,y_1)(c1​,y1​). These are the objects introduced on p. 91 of the paper.

For a generic cost-capital pair (c,y)(c,y)(c,y), production requires an external loan when cq>ycq>ycq>y. A competitive bank lends the shortfall cq−ycq-ycq−y and chooses a face value F(q)F(q)F(q) so that its expected receipt equals the loan principal. If sales revenue falls below the face value, the firm defaults; the bank recovers revenue less a proportion γ\gammaγ lost to bankruptcy, where γ∈[0,1]\gamma\in[0,1]γ∈[0,1]. The bank's zero-profit equation is equation (2), and Assumptions 2–3 require the adjusted face value to be below apapap and the face value to be below qpqpqp. A self-financed quantity has no loan. The firm's expected bankruptcy cost K(q)K(q)K(q) is the expected lost proportion of revenue in default. Its expected operating profit before the investment payment is

Jγ(c,y,q)=Eξ∼U[0,a][pmin⁡(q,ξ)]−cq−K(q).J_\gamma(c,y,q)=\mathbb E_{\xi\sim U[0,a]}[p\min(q,\xi)]-cq-K(q).Jγ​(c,y,q)=Eξ∼U[0,a]​[pmin(q,ξ)]−cq−K(q).

An equilibrium production quantity is any feasible q≥0q\ge0q≥0 that maximizes JγJ_\gammaJγ​ over every feasible nonnegative quantity. The mission compares equilibria for (c1,y1)(c_1,y_1)(c1​,y1​) and (c2,y2)(c_2,y_2)(c2​,y2​) at the same γ\gammaγ, then repeats the comparison at γ=0\gamma=0γ=0. Ties, if any, are allowed. The investment's net benefit Π(γ)\Pi(\gamma)Π(γ) is invested operating profit minus AAA minus noninvested operating profit. The model and profit definition follow equations (1)–(4) on p. 92 of the paper.

Formalization targets

The paper separates the net benefit into an operational effect ΔR1\Delta R_1ΔR1​, independent of γ\gammaγ, and a friction effect ΔR2(γ)\Delta R_2(\gamma)ΔR2​(γ):

Π(γ)=ΔR1+ΔR2(γ)−A.\Pi(\gamma)=\Delta R_1+\Delta R_2(\gamma)-A.Π(γ)=ΔR1​+ΔR2​(γ)−A.

Here ΔR1\Delta R_1ΔR1​ compares the perfect-market operating profits. Proposition 2 gives ΔR1=aβA(2p−2c1+βA)/(2p)>0\Delta R_1=a\beta A(2p-2c_1+\beta A)/(2p)>0ΔR1​=aβA(2p−2c1​+βA)/(2p)>0 in the positive-margin regime. Proposition 3 defines ΔR2\Delta R_2ΔR2​ by four integrals of the marginal rate of return MRR(q)=p(1−q/a)−c\mathrm{MRR}(q)=p(1-q/a)-cMRR(q)=p(1−q/a)−c and marginal cost of external funds MCE(q)=γcF(q)/(ap−(1+γ)F(q))\mathrm{MCE}(q)=\gamma cF(q)/(ap-(1+\gamma)F(q))MCE(q)=γcF(q)/(ap−(1+γ)F(q)). In particular, ΔR2\Delta R_2ΔR2​ is an explicit quantity derived from the two production and financing curves; it is not defined from the difference between Π(γ)\Pi(\gamma)Π(γ) and Π(0)\Pi(0)Π(0). These formulas appear on pp. 93–95 of the paper.

The goal is Proposition 4. For any positive γ≤1\gamma\le1γ≤1, at equilibrium quantities under friction and at their perfect-market counterparts, it states

ΔR2(γ)>0⟹Π(γ)>Π(0).\Delta R_2(\gamma)>0\quad\Longrightarrow\quad\Pi(\gamma)>\Pi(0).ΔR2​(γ)>0⟹Π(γ)>Π(0).

The milestone list follows the paper's supporting claims: competitive pricing of the loan, properties of bankruptcy cost and marginal financing cost, the equilibrium equations, the positive operational effect, the area description of profit, and the decomposition of Π\PiΠ. Each claim is stated over the same model. The goal makes no assertion that every parameter choice produces a positive friction effect; it identifies the consequence when the integral in equation (8) is positive.

What the result supplies

A positive ΔR2\Delta R_2ΔR2​ means the investment's change to production and financing improves its value relative to a perfect capital market. Proposition 4 turns that model-specific sign into a comparison of two net benefits, each evaluated at its own equilibrium quantities. Without the financing calculation, the direct reduction in unit cost alone says only that the operational effect is positive; it does not determine how market frictions change the investment's value. The distinction is the paper's contribution in §3 Tanrisever et al. (2021).

The result is proved in the published paper; its proofs are assigned there to Online Appendix A, which is not included in this mission's canonical PDF. This formalization sets up an open Lean proof problem for that known result. It also gives reusable, explicit definitions for competitive zero-profit loan pricing under uniform demand, proportional bankruptcy loss, feasible production, and equilibrium profit. Those definitions can support later formalizations of the paper's threshold and comparative-statics results. The local proposal contains statements and compiled definitions, while the milestone theorems and goal remain proof obligations.

Where the mathematical work lies

The comparison in Proposition 4 depends on an identity between two descriptions of profit. Equation (4) defines profit through expected revenue and the bankruptcy-cost expectation. Figures 2–3 and equation (8) express the same quantities through areas under marginal curves. Identifying the area with the expected-profit expression requires control of the loan face value as production varies and of the transition between borrowing and self-financed production. Merely subtracting the two profit formulas does not yield equation (8). The equilibrium quantity is also chosen over feasible production quantities determined by the bank's lending restrictions, so a stationary marginal equation needs justification as an equilibrium characterization. These are the main obligations represented by the earlier milestones.

Formalization scope and conventions

Lean uses real-valued parameters and a normalized interval integral, a−1∫0aa^{-1}\int_0^aa−1∫0a​, for every expectation under ξ∼U[0,a]\xi\sim U[0,a]ξ∼U[0,a]. The parameter record holds p,a,c1,y1,A,βp,a,c_1,y_1,A,\betap,a,c1​,y1​,A,β; a standing predicate requires their stated positivity, c2>0c_2>0c2​>0, and y2≥0y_2\ge0y2​≥0. The friction proportion remains a variable in [0,1][0,1][0,1]. Quantities are nonnegative with no imposed upper bound. Lending feasibility enforces Assumptions 2–3; self-financed quantities require no loan. Equilibrium quantities are hypotheses quantified over all feasible competitors, avoiding a default-valued supremum or a manufactured maximizer.

Two conventions are stated explicitly. First, c1<pc_1<pc1​<p is added for Propositions 2–4: with c1≥pc_1\ge pc1​≥p, the first upper limit in the paper's equation (8) can be negative, and its displayed implication fails. Second, F(q)=0F(q)=0F(q)=0 and MCE(q)=0\mathrm{MCE}(q)=0MCE(q)=0 where cq≤ycq\le ycq≤y. On the positive-loan branch, F(q)F(q)F(q) is the lower closed-form root of the bank's equation (2), and MCE\mathrm{MCE}MCE agrees with the printed formula. The paper usually assumes capital is insufficient for production; this proposal also allows self-financed production, with the convention disclosed in the statements. The definition of ΔR2\Delta R_2ΔR2​ is the four-integral equation (8), rather than Π(γ)−Π(0)\Pi(\gamma)-\Pi(0)Π(γ)−Π(0), and expected profit remains equation (4), rather than an area definition.

The development needs interval integration, real square roots and derivatives, convexity, and optimization over feasible real quantities from Mathlib. The definitions and theorems use the main text of the published article; proofs in its online appendices and the later numerical and stochastic extensions are outside the present scope.

Selected references

  • F. Tanrisever, N. Joglekar, S. Erzurumlu and M. Lévesque, Managing Capital Market Frictions via Cost-Reduction Investments, Manufacturing & Service Operations Management 23(1):88–105, 2021. DOI: 10.1287/msom.2019.0814.
9 thms2 active usersReviewed
Information TheoryQuantum Information·Captain: mikedeng1

General Benchmarks for Quantum Repeaters: For the Qudit Dephasing Channel the Entanglement-Flux Upper Bound Meets the Coherent Information, log₂ d − H(P)Research Paper

Motivation

A quantum repeater is judged by how much it beats direct transmission over a point-to-point link. The natural yardsticks are the two-way assisted capacities of the link's channel E\mathcal EE: the quantum capacity Q2(E)Q_2(\mathcal E)Q2​(E) and the secret-key capacity K(E)K(\mathcal E)K(E), the best rates of entanglement and key that two parties can obtain over many uses of E\mathcal EE when unlimited two-way classical communication and local operations are free. Computing them exactly for a given channel is rare, because it requires a lower and an upper bound that meet.

Pirandola and Laurenza (arXiv:1512.04945v2, 2016) obtain such matching bounds for a family of channels. The lower bound is the coherent information of the channel (with its reverse version), which is achievable by the hashing protocol. The upper bound is the entanglement flux Φ(E)\Phi(\mathcal E)Φ(E), the relative entropy of entanglement of the channel's Choi matrix, which bounds KKK for channels that can be simulated by teleportation. For the qudit dephasing channel the two bounds coincide, which gives Q2=K=log⁡2d−H(P)Q_2=K=\log_2 d-H(\mathbf P)Q2​=K=log2​d−H(P) (Eqs. (20) and (95)). This mission formalizes that coincidence.

Setting

Fix a dimension d≥2d\ge2d≥2 and the computational basis {∣j⟩}j=0d−1\{|j\rangle\}_{j=0}^{d-1}{∣j⟩}j=0d−1​ of a qudit. Let ω=e2πi/d\omega=e^{2\pi i/d}ω=e2πi/d and let ZZZ be the generalized phase operator, Z∣j⟩=ωj∣j⟩Z|j\rangle=\omega^j|j\rangleZ∣j⟩=ωj∣j⟩. For a dephasing probability p∈[0,1]p\in[0,1]p∈[0,1] define the binomial weights

Pm(p,d)=(d−1m)pm(1−p)d−1−m,m=0,…,d−1,P_m(p,d)=\binom{d-1}{m}p^m(1-p)^{d-1-m},\qquad m=0,\dots,d-1,Pm​(p,d)=(md−1​)pm(1−p)d−1−m,m=0,…,d−1,

and the qudit dephasing channel, given by its Kraus operators,

Pd(ρ)=∑m=0d−1EmρEm†,Em=Pm(p,d) Zm.\mathcal P_d(\rho)=\sum_{m=0}^{d-1}E_m\rho E_m^\dagger,\qquad E_m=\sqrt{P_m(p,d)}\,Z^m .Pd​(ρ)=m=0∑d−1​Em​ρEm†​,Em​=Pm​(p,d)​Zm.

Write P={Pm(p,d)}m\mathbf P=\{P_m(p,d)\}_mP={Pm​(p,d)}m​ and H(P)=−∑mPmlog⁡2PmH(\mathbf P)=-\sum_mP_m\log_2P_mH(P)=−∑m​Pm​log2​Pm​ (with 0log⁡0=00\log0=00log0=0) for its Shannon entropy.

The Choi matrix of a map E\mathcal EE on d×dd\times dd×d matrices is ρE=(I⊗E)(Ψd)\rho_{\mathcal E}=(\mathcal I\otimes\mathcal E)(\Psi_d)ρE​=(I⊗E)(Ψd​), where ∣Ψd⟩=d−1/2∑i∣ii⟩|\Psi_d\rangle=d^{-1/2}\sum_i|ii\rangle∣Ψd​⟩=d−1/2∑i​∣ii⟩. The first tensor factor is the reference RRR, the second the channel output BBB. With the von Neumann entropy S(ρ)=−Tr ρlog⁡2ρS(\rho)=-\mathrm{Tr}\,\rho\log_2\rhoS(ρ)=−Trρlog2​ρ:

  • the coherent information of the channel is IC(E)=S(TrRρE)−S(ρE)I_C(\mathcal E)=S(\mathrm{Tr}_R\rho_{\mathcal E})-S(\rho_{\mathcal E})IC​(E)=S(TrR​ρE​)−S(ρE​);
  • the reverse coherent information is IRC(E)=S(TrBρE)−S(ρE)I_{RC}(\mathcal E)=S(\mathrm{Tr}_B\rho_{\mathcal E})-S(\rho_{\mathcal E})IRC​(E)=S(TrB​ρE​)−S(ρE​);
  • the relative entropy is S(ρ∥σ)=Tr[ρ(log⁡2ρ−log⁡2σ)]S(\rho\|\sigma)=\mathrm{Tr}[\rho(\log_2\rho-\log_2\sigma)]S(ρ∥σ)=Tr[ρ(log2​ρ−log2​σ)], and +∞+\infty+∞ when the support of ρ\rhoρ is not inside that of σ\sigmaσ;
  • the relative entropy of entanglement of a bipartite state is ER(ρ)=inf⁡σ∈SEPS(ρ∥σ)E_R(\rho)=\inf_{\sigma\in\mathrm{SEP}}S(\rho\|\sigma)ER​(ρ)=infσ∈SEP​S(ρ∥σ), the infimum over all separable states for the cut R:BR:BR:B;
  • the entanglement flux of the channel is Φ(E)=ER(ρE)\Phi(\mathcal E)=E_R(\rho_{\mathcal E})Φ(E)=ER​(ρE​).

The paper's candidate separable state is σ~=∑i1d∣i⟩⟨i∣⊗Pd(∣i⟩⟨i∣)\tilde\sigma=\sum_i\frac1d|i\rangle\langle i|\otimes\mathcal P_d(|i\rangle\langle i|)σ~=∑i​d1​∣i⟩⟨i∣⊗Pd​(∣i⟩⟨i∣).

Formalization targets

Goal (Eqs. (94)–(95), p. 11)

For every d≥2d\ge2d≥2 and p∈[0,1]p\in[0,1]p∈[0,1]:

IC(Pd)=IRC(Pd)=log⁡2d−H(P),Φ(Pd)≤log⁡2d−H(P).I_C(\mathcal P_d)=I_{RC}(\mathcal P_d)=\log_2d-H(\mathbf P),\qquad \Phi(\mathcal P_d)\le\log_2d-H(\mathbf P).IC​(Pd​)=IRC​(Pd​)=log2​d−H(P),Φ(Pd​)≤log2​d−H(P).

The lower and the upper bound on the two-way capacities therefore meet. The statement keeps ddd and ppp free and asserts exact values, not numerical constants.

Milestones (in attack order)

  1. The Choi matrix of Pd\mathcal P_dPd​ in closed form (p. 11, display between Eqs. (90) and (91)).
  2. Eq. (91): S(ρPd)=H(P)S(\rho_{\mathcal P_d})=H(\mathbf P)S(ρPd​​)=H(P).
  3. Eq. (68): S(ρ∥σ)=−S(ρ)−∑i⟨i∣ρ∣i⟩log⁡siS(\rho\|\sigma)=-S(\rho)-\sum_i\langle i|\rho|i\rangle\log s_iS(ρ∥σ)=−S(ρ)−∑i​⟨i∣ρ∣i⟩logsi​ in the eigenbasis of σ\sigmaσ, under support inclusion.
  4. Eq. (92): σ~=∑i1d∣ii⟩⟨ii∣\tilde\sigma=\sum_i\frac1d|ii\rangle\langle ii|σ~=∑i​d1​∣ii⟩⟨ii∣ and σ~\tilde\sigmaσ~ is separable.
  5. Eq. (93): Tr(ρPdlog⁡2σ~)=−log⁡2d\mathrm{Tr}(\rho_{\mathcal P_d}\log_2\tilde\sigma)=-\log_2dTr(ρPd​​log2​σ~)=−log2​d, with the support of ρPd\rho_{\mathcal P_d}ρPd​​ inside that of σ~\tilde\sigmaσ~.
  6. Eq. (94): Φ(Pd)≤S(ρPd∥σ~)=log⁡2d−H(P)\Phi(\mathcal P_d)\le S(\rho_{\mathcal P_d}\|\tilde\sigma)=\log_2d-H(\mathbf P)Φ(Pd​)≤S(ρPd​​∥σ~)=log2​d−H(P).
  7. Eq. (45): for a unital, trace-preserving map E\mathcal EE, IC(E)=IRC(E)=log⁡2d−S(ρE)I_C(\mathcal E)=I_{RC}(\mathcal E)=\log_2d-S(\rho_{\mathcal E})IC​(E)=IRC​(E)=log2​d−S(ρE​).

Significance

The result. The coincidence of the two bounds pins down Q2Q_2Q2​ and KKK of the qudit dephasing channel for every ddd and ppp, which gives the repeaterless benchmark for any qudit link dominated by dephasing. At d=2d=2d=2 it recovers the qubit dephasing benchmark 1−H2(p)1-H_2(p)1−H2​(p) of the same paper (Eq. (75), with p↔1−pp\leftrightarrow1-pp↔1−p, which the binary entropy does not see). Combined with the operational facts the paper imports (the hashing inequality and the bound of KKK by the flux for teleportation-covariant channels), it yields the capacity formula (95).

Formalizing it. The paper's computation is complete but terse. The formalization makes three implicit points explicit: the support of the Choi matrix lies inside the support of the rank-ddd state σ~\tilde\sigmaσ~ (so log⁡σ~\log\tilde\sigmalogσ~ is taken on its support); the claim of "ddd non-zero eigenvalues" in (91) fails at p∈{0,1}p\in\{0,1\}p∈{0,1}, while the entropy identity does not; and (45) needs trace preservation as well as unitality. The results are proved in the paper and, as far as the platform's catalogue shows, formalized nowhere. Eq. (68) and Eq. (45) are reusable lemmas about arbitrary states and unital channels.

Difficulty

The calculation on the page is short; the difficulty lies in what it leaves to the reader. The entropy identity (91) asks for the spectrum of a d2×d2d^2\times d^2d2×d2 matrix that is not diagonal in the computational basis, while the von Neumann entropy is defined through the matrix functional calculus, so "diagonalizing" has to be made precise. The state σ~\tilde\sigmaσ~ has rank ddd in dimension d2d^2d2: the relative entropy against it is finite only because of a support inclusion the paper does not mention, and a computation that ignores the kernel of σ~\tilde\sigmaσ~ does not establish the value. The upper bound needs σ~\tilde\sigmaσ~ to be separable in the sense of the infimum, a finite convex combination of product density matrices, not merely diagonal. Finally, the coherent information is a difference of entropies of a partial trace and of the full Choi matrix; equating it to log⁡2d−H(P)\log_2 d-H(\mathbf P)log2​d−H(P) requires both that the output marginal is maximally mixed and the entropy identity (91).

Formalization scope

Qudit indices are Fin d, with d≥2d\ge2d≥2 (and [NeZero d] where an instance needs it); ppp is real with 0≤p≤10\le p\le10≤p≤1. ZmZ^mZm is a matrix power, ω=exp⁡(2πi/d)\omega=\exp(2\pi i/d)ω=exp(2πi/d), and the channel is the published QAlgorithms.krausApply of the Kraus family Pm Zm\sqrt{P_m}\,Z^mPm​​Zm. The Choi matrix is the published QAlgorithms.idTensorSuperop applied to maximallyEntangledProjector d (entries 1/d1/d1/d on ∣ii⟩⟨jj∣|ii\rangle\langle jj|∣ii⟩⟨jj∣), the reference being the first factor of Fin d × Fin d. Entropies are in bits with 0log⁡0=00\log0=00log0=0: QAlgorithms.vnEntropy for states and a local Shannon entropy for the weights. The partial traces are QAlgorithms.traceLeft (over the reference) and QAlgorithms.traceRight (over the output). The relative entropy and ERE_RER​ are the published relativeEntropyBits and relativeEntanglement (Umegaki entropy divided by ln⁡2\ln2ln2, +∞+\infty+∞ off support, infimum over IsSeparableDensity, values in [0,∞][0,\infty][0,∞]). The real bound is embedded with ENNReal.ofReal; since H(P)≤log⁡2dH(\mathbf P)\le\log_2dH(P)≤log2​d, nothing is lost.

None of the defined quantities is given by its closed form: the Choi matrix is computed from the channel, ERE_RER​ is the infimum over all separable states (not S(ρ∥σ~)S(\rho\|\tilde\sigma)S(ρ∥σ~) or an infimum over diagonal states), and ICI_CIC​ is defined from partial traces, not as log⁡2d−S(ρE)\log_2d-S(\rho_{\mathcal E})log2​d−S(ρE​). This rules out the trivializing formalization in which a milestone or the goal holds by definition. The bound log⁡2d\log_2dlog2​d alone holds for every state; the goal's bound is log⁡2d−H(P)\log_2d-H(\mathbf P)log2​d−H(P).

The operational capacities Q2Q_2Q2​ and KKK of Eq. (95) are not formalized. They are defined over adaptive LOCC protocols with private-state targets, which have no substrate on the platform. The paper also does not prove the two bridges from them to the bounds: it imports K≤ΦK\le\PhiK≤Φ (Eq. (2), from Pirandola et al.) and the hashing inequality (from Devetak and Winter). For the same reason, the reverse inequality Φ(Pd)≥log⁡2d−H(P)\Phi(\mathcal P_d)\ge\log_2d-H(\mathbf P)Φ(Pd​)≥log2​d−H(P) is not stated, since the paper obtains it only through the hashing bound. Teleportation stretching, convexity of the flux, the bosonic Gaussian channels and the erasure channel are outside this mission.

Contributions are welcome at every level: the spectrum of circulant blocks, the support calculus of the Umegaki entropy, and the separable decomposition of diagonal states are all reusable beyond this mission.

Selected references

  • S. Pirandola, R. Laurenza, General Benchmarks for Quantum Repeaters, arXiv preprint, v2, 2016. https://arxiv.org/abs/1512.04945v2
  • S. Pirandola, R. Laurenza, C. Ottaviani, L. Banchi, Fundamental limits of repeaterless quantum communications, Nature Communications 8, 15043, 2017. https://doi.org/10.1038/ncomms15043
  • I. Devetak, A. Winter, Distillation of secret key and entanglement from quantum states, Proc. R. Soc. A 461, 207–235, 2005. https://doi.org/10.1098/rspa.2004.1372
  • V. Vedral, M. B. Plenio, Entanglement measures and purification procedures, Phys. Rev. A 57, 1619, 1998. https://doi.org/10.1103/PhysRevA.57.1619
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Bandit AlgorithmsOperations ResearchProbability·Captain: mikedeng1

A Note on the Equivalence of Upper Confidence Bounds and Gittins Indices for Patient Agents: The Gaussian Gittins Index Equals the Posterior γ-Quantile μ + Φ⁻¹(γ)σ up to o(1) as γ → 1Research Paper

Motivation

A Gittins index assigns a number to an uncertain arm in a discounted bandit problem. The index converts a sequential choice, where an agent may keep gathering information or retire, into a tax threshold for playing the arm. Computing it generally requires an optimal stopping calculation. A Bayesian upper confidence bound, by comparison, is a quantile of the posterior distribution and is directly available for a Gaussian posterior. Russo's note asks how closely these two quantities agree when the agent is patient and the discount factor approaches one. The answer is an asymptotic identity for a Gaussian arm, not a finite-discount formula. Russo, 2019, pp. 1–3.

The note places its result alongside work on computational approximations of Gittins indices and finite-horizon index policies, but aims at the conceptual relationship with Bayesian confidence bounds. It appeared as an arXiv preprint in 2019; this mission follows that version's theorem numbering and formulas. A later journal publication appeared in Operations Research in 2021, but its numbering is not used here.

Setting

One arm has an unknown quality θ\thetaθ. The prior distribution is Gaussian, θ∼N(μ,σ2)\theta\sim N(\mu,\sigma^2)θ∼N(μ,σ2), where μ∈R\mu\in\mathbb Rμ∈R and σ2>0\sigma^2>0σ2>0. Playing the arm at time ttt yields Rt=θ+WtR_t=\theta+W_tRt​=θ+Wt​, where the observation noises WtW_tWt​ are independent Gaussian variables of mean zero and variance σW2>0\sigma_W^2>0σW2​>0. After observing R0,…,Rt−1R_0,\ldots,R_{t-1}R0​,…,Rt−1​, the posterior is N(μt,σt2)N(\mu_t,\sigma_t^2)N(μt​,σt2​). Its mean and variance follow the Gaussian update (1) of Russo, p. 2. In particular, σt2=(1/σ2+t/σW2)−1\sigma_t^2=(1/\sigma^2+t/\sigma_W^2)^{-1}σt2​=(1/σ2+t/σW2​)−1.

For each play, the agent pays a tax λ∈R\lambda\in\mathbb Rλ∈R. The agent may retire, receiving zero thereafter. At discount factor 0<γ<10<\gamma<10<γ<1, an admissible retirement time τ≥1\tau\ge1τ≥1 uses only the rewards observed through the current time. Its discounted payoff includes the play at τ\tauτ: ∑t=0τγt(θ−λ)\sum_{t=0}^{\tau}\gamma^t(\theta-\lambda)∑t=0τ​γt(θ−λ). The value Vγλ(μ,σ2;σW2)V^\lambda_\gamma(\mu,\sigma^2;\sigma_W^2)Vγλ​(μ,σ2;σW2​) is the supremum of the expected payoff over these retirement times. The Gittins index λγ(μ,σ2;σW2)\lambda_\gamma(\mu,\sigma^2;\sigma_W^2)λγ​(μ,σ2;σW2​) is the supremum of taxes for which the value is nonnegative. These are the stopping-time value and fair-tax definition in equations (2)–(3) of Russo, p. 2.

Write Φ\PhiΦ and ϕ\phiϕ for the distribution function and density of N(0,1)N(0,1)N(0,1), and Φ−1(γ)=inf⁡{z:Φ(z)≥γ}\Phi^{-1}(\gamma)=\inf\{z:\Phi(z)\ge\gamma\}Φ−1(γ)=inf{z:Φ(z)≥γ}. Thus μ+σΦ−1(γ)\mu+\sigma\Phi^{-1}(\gamma)μ+σΦ−1(γ) is the prior's upper γ\gammaγ-quantile, with σ=σ2\sigma=\sqrt{\sigma^2}σ=σ2​.

Formalization targets

Gaussian Gittins index asymptotic

The goal is Theorem 1, p. 3, for each fixed prior mean, positive prior variance, and positive observation-noise variance:

λγ(μ,σ2;σW2)=μ+σΦ−1(γ)+o(1)(γ↑1).\lambda_\gamma(\mu,\sigma^2;\sigma_W^2) =\mu+\sigma\Phi^{-1}(\gamma)+o(1) \qquad(\gamma\uparrow1).λγ​(μ,σ2;σW2​)=μ+σΦ−1(γ)+o(1)(γ↑1).

The remainder is an additive quantity tending to zero; the claim does not assert equality at any fixed discount factor. The paper reduces the general prior to a standardized one. Its intermediate targets are the normal-quantile asymptotic, explicit bounds on E[(X−λ)+]\mathbb E[(X-\lambda)^+]E[(X−λ)+], an upper bound obtained from noiseless information, and a matching lower bound from an admissible exploration policy. They appear as the mission's milestones, along with the posterior identities the lower bound uses. Russo, pp. 3–6.

Significance

The theorem identifies the limiting tax threshold with a familiar statistical quantile. It explains why a Bayesian upper confidence bound can approximate the Gittins priority of an arm when the effective horizon is large. It does not state that a quantile policy is exactly optimal at a fixed horizon or discount factor, and the paper's limitations section notes that significant observation noise relative to the horizon can make exploration costly. Russo, pp. 3, 7.

For a formal development, the reusable pieces are a Gaussian stopping-time model, the fair-tax index, the normal tail and positive-part estimates, and posterior update identities. The asymptotic theorem is proved in the source paper but has no machine-checked proof in this mission. Its local Lean statement is a target with sorry; the same applies to the milestone theorems. The definitions and a small sanity lemma compile in the pinned environment. Contributions that establish the source's stated bounds, their probabilistic prerequisites, or the final asymptotic reduction are relevant.

Difficulty

The direct idea of replacing the index by a posterior quantile at each fixed γ\gammaγ does not establish the theorem. The index optimizes over retirement times that adapt to noisy observations. A decision maker who sees θ\thetaθ without noise has a larger value, so the resulting expression supplies an upper bound, but it does not give a lower bound for the original information structure. The paper's matching lower estimate uses an actual reward-adapted policy and tracks both the cost of initial sampling and the benefit of later commitment. The two estimates must agree to an additive o(1)o(1)o(1), not merely at their leading order. Russo, §§3.3–3.4, pp. 4–7.

Formalization scope

Lean uses the canonical probability space Ω=R×(N→R)\Omega=\mathbb R\times(\mathbb N\to\mathbb R)Ω=R×(N→R): the first coordinate is θ\thetaθ, and the second is the independent noise sequence. The model measure is the Gaussian prior times an infinite product of Gaussian noise laws. The reward history at time ttt generates Ft=σ(R0,…,Rt)\mathcal F_t=\sigma(R_0,\ldots,R_t)Ft​=σ(R0​,…,Rt​). An admissible N∞\mathbb N_\inftyN∞​-valued stopping time has τ≥1\tau\ge1τ≥1; τ=∞\tau=\inftyτ=∞ means never retire. The stopped reward is a countable sum. The index is the supremum of the nonnegative-value tax set. Only the discount domain 0<γ<10<\gamma<10<γ<1 is used in fixed-discount statements; limits approach one from below. Variances are nonnegative reals at the Mathlib Gaussian interface, with strict positivity assumed in the theorem statements. The paper suppresses σW2\sigma_W^2σW2​ in the index notation; Lean keeps it explicit and arbitrary.

The value is defined from the stopping problem and the index from the fair-tax set. Retirement decisions depend on observed rewards only; giving them access to θ\thetaθ would change the target. The posterior variance uses t/σW2t/\sigma_W^2t/σW2​ in its closed form, correcting a printed error in (1). Lemma 3's limit is γ↑1\gamma\uparrow1γ↑1, and Lemma 7 uses log⁡(1/(1−γ))\log(1/(1-\gamma))log(1/(1−γ)) in its little-o scale; their printed versions are inconsistent with the surrounding derivations. The natural-language item notes identify these corrections. Russo, pp. 2, 4, 6, 9.

Selected references

  • Daniel Russo, A Note on the Equivalence of Upper Confidence Bounds and Gittins Indices for Patient Agents, arXiv:1904.04732v1, 2019. Preprint.
  • J. C. Gittins, K. D. Glazebrook, and R. Weber, Multi-Armed Bandit Allocation Indices, 2nd ed., Wiley, 2011. DOI.
13 thms2 active usersReviewed
Mathematical PhysicsProbabilityQuantum Information·Captain: mikedeng1

Large Deviations in Quantum Spin Chain: Full Large Deviation Principle with a Good Rate Function for C*-Finitely Correlated StatesResearch Paper

Motivation

Measurements of long quantum spin chains can have outcomes far from their typical values. A large-deviation principle quantifies how quickly the probability of such outcomes decreases with the number of sites. In a classical lattice system this is a standard way to describe rare macroscopic fluctuations; in a quantum chain, observables on overlapping sets of sites generally fail to commute, which makes the corresponding probability laws harder to analyze. Ogata's 2008 paper establishes a full principle for the energy density of any translation-invariant finite-range interaction in a C∗C^*C∗-finitely correlated state. Its introduction explains that earlier spin-chain results covered upper bounds or more restricted observables and states, while the lower bound for general observables remained the substantial issue. Ogata, pp. 2–4

The finitely correlated class includes local states generated from finite auxiliary memory. It is large enough to include mixtures and periodic behavior, so a theorem restricted to a primitive transfer map would miss part of Ogata's statement. This mission targets the printed Theorem 1.2 in its full scope. Ogata, p. 4

Setting

At each site let Md(C)M_d(\mathbb C)Md​(C) be the algebra of complex d×dd\times dd×d matrices. On sites 1,…,n1,\ldots,n1,…,n, the local algebra is the nnn-fold tensor product, represented as matrices whose rows and columns are spin configurations. A finite-range translation-invariant interaction Φ\PhiΦ assigns a Hermitian operator Φ(X)\Phi(X)Φ(X) to each finite set of sites X⊂ZX\subset\mathbb ZX⊂Z, with the same term on translated sets and with Φ(X)=0\Phi(X)=0Φ(X)=0 when the diameter of XXX exceeds a fixed range. Its finite-volume Hamiltonian is

HΦ([1,n])=∑X⊆[1,n]Φ(X).H_\Phi([1,n])=\sum_{X\subseteq[1,n]}\Phi(X).HΦ​([1,n])=X⊆[1,n]∑​Φ(X).

The sum includes the scalar term associated with the empty set. The interaction need not be nearest-neighbor and may have a term on any finite pattern within its range. Ogata, pp. 2–3

A C∗C^*C∗-finitely correlated state is specified by a finite-dimensional auxiliary algebra B\mathcal BB, a unital completely positive map E:Md(C)⊗B→B\mathcal E:M_d(\mathbb C)\otimes\mathcal B\to\mathcal BE:Md​(C)⊗B→B, and a faithful stationary state ρ\rhoρ on B\mathcal BB. Iterating E\mathcal EE gives a compatible local state ωn\omega_nωn​ on nnn sites. The probability measure μn,Φ\mu_{n,\Phi}μn,Φ​ is the spectral distribution of HΦ([1,n])/nH_\Phi([1,n])/nHΦ​([1,n])/n in ωn\omega_nωn​: for a Borel set B⊆RB\subseteq\mathbb RB⊆R, it assigns the state weight of the spectral projection corresponding to BBB. These local restrictions determine the distributions used in the theorem. Ogata, pp. 3–4

Formalization targets

Full large-deviation principle

The goal is a good rate function I:R→[0,∞]I:\mathbb R\to[0,\infty]I:R→[0,∞]: III is lower semicontinuous and each set {x:I(x)≤a}\{x:I(x)\le a\}{x:I(x)≤a} is compact for finite a≥0a\ge0a≥0. For every closed CCC and open OOO in R\mathbb RR, Theorem 1.2 asserts

lim sup⁡n→∞1nlog⁡μn,Φ(C)≤−inf⁡x∈CI(x),\limsup_{n\to\infty}\frac1n\log\mu_{n,\Phi}(C)\le-\inf_{x\in C}I(x),n→∞limsup​n1​logμn,Φ​(C)≤−x∈Cinf​I(x), lim inf⁡n→∞1nlog⁡μn,Φ(O)≥−inf⁡x∈OI(x).\liminf_{n\to\infty}\frac1n\log\mu_{n,\Phi}(O)\ge-\inf_{x\in O}I(x).n→∞liminf​n1​logμn,Φ​(O)≥−x∈Oinf​I(x).

One rate function serves both inequalities and every eligible set. The statement asserts existence, without imposing a formula for III or a primitivity condition on the auxiliary map. Ogata, pp. 3–4

Supporting targets

The milestone list includes the paper's Gärtner–Ellis theorem, the spectral-law exponential-moment identity behind equation (1), the two-sided order estimate (15) for a gapped auxiliary map, the regrouping of lll consecutive sites into one site, under which the same state is generated by the lll-th iterate E(l)\mathcal E^{(l)}E(l) of the transfer map and E(l)^1=(E^1)l\widehat{\mathcal E^{(l)}}_1=(\widehat{\mathcal E}_1)^lE(l)1​=(E1​)l, and the differentiable limiting pressure under condition (14). In the last target, the pressure is the limit of n−1log⁡ωn(eαHΦ([1,n]))n^{-1}\log\omega_n(e^{\alpha H_\Phi([1,n])})n−1logωn​(eαHΦ​([1,n])) for every real α\alphaα. These are narrower claims with separate hypotheses; none replaces the full goal. Ogata, pp. 4–5, 12–15

Significance

The theorem gives an exponential-scale description of the energy-density distribution for all translation-invariant finite-range interactions in this state class. The upper bound controls probability on closed sets; the lower bound supplies the matching guarantee for open sets. Compact sublevel sets prevent low-rate mass from escaping to infinity. The result is already proved in Ogata's paper; the remaining work here is a machine-checked development of the statement and its supporting mathematics. Ogata, Theorem 1.2

Formalizing the finite-dimensional transfer construction, its spectral measures, and an extended-valued LDP vocabulary would also make these objects available for later spin-chain results. The goal itself is not currently accompanied by a machine-checked proof in this mission. The Gärtner–Ellis and auxiliary-map statements are likewise proof targets, not asserted as solved Lean facts.

Difficulty

The exponential of a sum of overlapping local interaction terms cannot generally be factored into independent one-site contributions. Even when an auxiliary transfer map has a spectral gap and yields a differentiable limiting pressure, that argument does not directly cover every finitely correlated state. A mixture can have a limiting log moment generating function with a corner; the resulting rate function can be nonconvex. Ogata's printed Lemma 4.1 reduces to special components but omits the separate mixture step needed to recover the unrestricted theorem. The goal retains the theorem's printed hypotheses, while the condition-(14) milestone records precisely the restricted pressure claim. Ogata, pp. 12–15

Formalization scope

The Lean model uses finite matrices for local algebras. A nonempty finite site basis represents Md(C)M_d(\mathbb C)Md​(C), with site 1 indexed by 0. An interaction stores one Hermitian term for each support anchored at its least site; all translates that fit in [1,n][1,n][1,n] appear in the Hamiltonian. The scalar empty-set term is retained. The auxiliary algebra is represented by a full matrix algebra Mk(C)M_k(\mathbb C)Mk​(C); finite-dimensional C∗C^*C∗-algebra data have an equivalent full-matrix representation for the generated local states. Stationarity is written in the primal trace form. The recursive local state places the first site's matrix in the outermost application of E\mathcal EE.

The spectral law is formed from the eigenvalues and spectral weights of the actual Hamiltonian. It is not supplied as an arbitrary sequence of measures. The theorem uses no ergodicity, spectral-gap, or condition-(14) binder, and both LDP bounds range over every closed or open subset of R\mathbb RR. Logarithms of probabilities take values in the extended reals, with log⁡0=−∞\log0=-\inftylog0=−∞; sequence limits are at n→∞n\to\inftyn→∞, so the placeholder value at n=0n=0n=0 is immaterial. Nonnegative lower integrals represent exponential moments. In the restricted pressure milestone, the real logarithm applies to a positive state expectation. These choices also rule out a vacuous proof based on a zero measure, a moment represented by a non-integrable Bochner integral, or a rate function unrelated to the spectral law.

Reusable contributions include finite-dimensional spectral-law lemmas, positivity and stationarity facts for completely positive maps, good-rate-function and LDP lemmas on R\mathbb RR, and the Gärtner–Ellis result. The full theorem additionally needs a treatment of non-ergodic finite mixtures and periodic components that preserves both large-deviation bounds.

Selected references

  • Yoshiko Ogata, Large Deviations in Quantum Spin Chain, arXiv preprint, 2008. arXiv:0803.0113v1.
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A No-Go Theorem for Gaussian Quantum Error Correction: Gaussian Encoding and Decoding Cannot Lower the Entanglement Degradation of a Single-Mode Gaussian ChannelResearch Paper

Motivation

Optical quantum communication commonly encodes information in continuous variables such as the position and momentum quadratures of a light mode. Gaussian states and Gaussian operations are attractive in this setting because phase shifters, squeezers, beam splitters, and homodyne measurements are standard optical tools. Transmission through a lossy or noisy line can also be modeled by a Gaussian channel. The practical question is whether adding vacuum modes and Gaussian encoding and decoding can protect a signal against such a channel. Niset, Fiurášek, and Cerf (2008) give a negative answer for the code class defined in their Fig. 1.

The result sits after the early impossibility results for distilling Gaussian entanglement with Gaussian operations, including Giedke and Cirac (2002). Those results concern shared states and allowed local operations. The 2008 paper asks the channel-coding question directly: whether a finite Gaussian code can make a fixed single-mode Gaussian channel less damaging to entanglement. It introduces a scalar, entanglement degradation, to state the answer for every single-mode Gaussian channel in one inequality.

Setting

A single optical mode has two real quadratures, xxx and ppp. For nnn modes, the order is (x1,p1,…,xn,pn)(x_1,p_1,\ldots,x_n,p_n)(x1​,p1​,…,xn​,pn​). A state has a real covariance matrix γ\gammaγ recording its second moments in this order. The vacuum covariance matrix is the identity III. A Gaussian channel TTT on one mode is described at the covariance level by two real 2×22\times22×2 matrices MMM and NNN:

γ⟼MγMT+N.\gamma\longmapsto M\gamma M^{\mathsf T}+N.γ⟼MγMT+N.

Here NNN is the added noise. Complete positivity imposes symmetry and a matrix positivity condition on NNN; in particular, it gives det⁡N≥(det⁡M−1)2\det N\ge(\det M-1)^2detN≥(detM−1)2. A Gaussian unitary changes covariances by a symplectic matrix SSS, satisfying SJST=JSJS^{\mathsf T}=JSJST=J for the canonical symplectic form JJJ. Displacements affect first moments only and therefore play no role in these covariance formulas.

The code G(n,E,D)G(n,E,D)G(n,E,D) uses a positive integer nnn. The input occupies mode zero in the formalization; the other n−1n-1n−1 modes are vacuum ancillas. A Gaussian encoding unitary EEE acts on all modes, then the same channel TTT acts independently once on each mode, and a Gaussian decoding unitary DDD acts on all modes. Only the first output mode is retained. This defines an effective single-mode channel TGCT_{GC}TGC​ with matrices MGC,NGCM_{GC},N_{GC}MGC​,NGC​. The ancillas contribute noise to NGCN_{GC}NGC​ even before the nnn channel uses are counted.

For a channel T=(M,N)T=(M,N)T=(M,N), the paper defines its degradation by

D[T]=min⁡{det⁡N(1+det⁡M)2,1}.D[T]=\min\left\{\frac{\det N}{(1+\det M)^2},1\right\}.D[T]=min{(1+detM)2detN​,1}.

The intended value is 111 when the denominator vanishes: the quotient is then interpreted as infinite and is saturated by the minimum. This quantity is related to the entanglement remaining when TTT acts on one half of a two-mode squeezed vacuum as the squeezing grows. The paper measures that entanglement through the smallest symplectic eigenvalue ν−\nu_-ν−​ after partial transpose and the logarithmic negativity EN=max⁡{0,−log⁡ν−}E_N=\max\{0,-\log\nu_-\}EN​=max{0,−logν−​}.

Formalization targets

Main no-go theorem

The mission goal is the theorem on page 3, equation (11): for every completely positive single-mode Gaussian channel and every finite code of the stated form,

D[T]≤D[TGC].D[T]\le D[T_{GC}].D[T]≤D[TGC​].

This is the assertion that the code cannot lower the channel's entanglement degradation. It includes n=1n=1n=1, singular channels, and channels with negative determinant MMM. No numerical performance constant or bound on the number of modes is fixed.

Supporting results

The milestones record the paper's channel-noise constraint (2), the fact that the code produces a Gaussian channel, the local matrix normal forms used in Lemma 2, the asymptotic calculations (8) and (10), the entanglement-breaking case, and Lemma 2 itself. Lemma 2 characterizes the degradation through the limiting squared eigenvalue and, when finite, gives EN=−12log⁡D[T]E_N=-\tfrac12\log D[T]EN​=−21​logD[T]. The milestones retain the paper's distinction between positive, negative, and zero determinant regimes.

Significance

The theorem rules out a specific and broad way of improving Gaussian transmission: adding any finite number of vacuum ancillas and using Gaussian unitaries before and after independent uses of a fixed channel cannot improve this intrinsic entanglement measure. The paper applies this conclusion to attenuation, amplification, and classical-noise channels, showing how an apparent reduction in one channel parameter can be offset by increased noise. It also relates degradation to an upper bound on quantum capacity, though that further bound is outside this mission. Niset, Fiurášek, and Cerf (2008)

The paper's theorem is proved in the mathematical literature; the goal here is a machine-checked statement and, eventually, a proof in the covariance-matrix representation. The published covariance layer already supplies symplectic forms, two-mode squeezed covariances, partial transpose, and an intrinsic ν−\nu_-ν−​; this mission adds the channel and code definitions required to state the no-go theorem. Those definitions can be reused for other single-mode Gaussian-channel questions. A complete proof still needs substantial results connecting codes, Gaussian operations, and entanglement behavior; a compiled sorry statement alone does not establish the theorem.

Difficulty

One might try to compare det⁡N\det NdetN before and after the code. That scalar does not track the code: encoding mixes signal and vacuum modes, each copy of the channel adds noise, decoding mixes the modes again, and discarding modes changes both MGCM_{GC}MGC​ and NGCN_{GC}NGC​. Neither determinant separately gives the desired inequality. The boundary det⁡M=−1\det M=-1detM=−1 also defeats a direct real-valued transcription of the printed quotient. The asymptotic entanglement formulas cross several determinant regimes, with different normal forms and a separate entanglement-breaking case. The central challenge is to retain the physical meaning of all these cases in one theorem over arbitrary finite codes.

Formalization scope

Lean uses real matrices indexed by interleaved mode and quadrature coordinates. The published QAlgorithms_Papers_Independent_Frontier30_P13 layer provides ModeQuadrature, phaseJ, squeezedCM, partial transpose, and the intrinsic smallest symplectic eigenvalue lambdaMin; QAlgorithms_Papers_Independent_Dependency50_P10 provides entrywise complexification. A channel is required to satisfy the Gaussian complete-positivity matrix inequality. Encoders and decoders satisfy SJST=JSJS^{\mathsf T}=JSJST=J. The code uses the same (M,N)(M,N)(M,N) on every one of its nnn modes, with n≥1n\ge1n≥1, and includes the vacuum covariance on every ancillary mode. Gaussian unitaries enter through their symplectic matrices; their displacement parts do not affect covariances.

The definition of DDD explicitly saturates at 111 when 1+det⁡M=01+\det M=01+detM=0, avoiding Lean's zero value for division by zero. The squeezed input uses cosh⁡(2r)\cosh(2r)cosh(2r) and sinh⁡(2r)\sinh(2r)sinh(2r). The eigenvalue ν−\nu_-ν−​ is the intrinsic lambdaMin, not an unguarded square-root expression. Logarithmic negativity uses the natural logarithm; its finite limit statement assumes det⁡N>0\det N>0detN>0, while the degradation statement still covers det⁡N=0\det N=0detN=0. The infinite-squeezing output is represented by limits of finite-rrr covariances and entanglement quantities.

The code's vacuum term, all nnn noise blocks, the symplectic equation, and the guarded degradation are essential to the target; dropping any of them would change the question. Lemma 1's teleportation equivalence and the external Gaussian no-distillation theorem are not formalized here. Their faithful treatment would require operational Gaussian states, measurements, and protocols beyond the covariance model. Contributions establishing those interfaces, proving the stated matrix milestones, or connecting the two layers are welcome.

Selected references

  • J. Niset, J. Fiurášek, and N. J. Cerf, A No-Go Theorem for Gaussian Quantum Error Correction, Physical Review Letters 102, 120501, 2009; arXiv:0811.3128v1 (2008). The preprint is the citation basis for page and equation numbers here.
  • G. Giedke and J. I. Cirac, Characterization of Gaussian operations and distillation of Gaussian states, Physical Review A 66, 032316, 2002; arXiv:quant-ph/0204085.
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Qudit circuits with SU(d) symmetry: Locality imposes additional conservation laws: Tr(Ω[ρ]^l) is conserved by every unitary generated by 2-local SU(d)-invariant gatesResearch Paper

Motivation

Quantum circuits whose gates respect a global symmetry are a standard model for quantum simulation, for symmetry-protected quantum computing, and for the study of conserved quantities in quantum dynamics. For SU(d) symmetry on nnn qudits, the unitaries that commute with every U⊗nU^{\otimes n}U⊗n are, by Schur–Weyl duality, exactly the unitaries in the linear span of the qudit permutations. A natural question is whether every such unitary can be built from local symmetric gates, as happens without symmetry, where 2-qudit gates are universal.

Marvian, Liu and Hulse (arXiv:2105.12877) show that for d≥3d \ge 3d≥3 the answer is no, and that the obstruction appears as conservation laws. Unitaries generated by 2-local SU(d)-invariant gates conserve quantities that general SU(d)-invariant unitaries change. The paper gives two families of such laws. The first, Theorem 1 (the fsgnf_{\mathrm{sgn}}fsgn​ law, from a Z2\mathbb Z_2Z2​ symmetry of the swap Hamiltonians), is a separate result of the paper and is not part of this mission. The second, Theorem 2, is the target here. It comes from a correspondence between a subspace of the qudits and a system of free fermions.

Timeline: Marvian (Nature Physics 18, 283, 2022) showed that symmetry together with locality restricts the realizable unitaries in general, with examples for U(1) and SU(2) symmetry. For qubits with SU(2) symmetry, the constraints restrict only relative phases between sectors of inequivalent irreducible representations (p. 3 of the present paper). The present paper (arXiv:2105.12877, v2 January 2022) treats SU(d) with d≥3d\ge 3d≥3, where constraints beyond relative phases appear. The connection to Marin's 2007 description of the Lie algebra generated by transpositions (J. Algebra 310, 742) is discussed on p. 9.

Setting

Consider nnn qudits with Hilbert space (Cd)⊗n(\mathbb C^d)^{\otimes n}(Cd)⊗n and computational basis ∣x1⟩⋯∣xn⟩|x_1\rangle\cdots|x_n\rangle∣x1​⟩⋯∣xn​⟩, xi∈{0,…,d−1}x_i\in\{0,\dots,d-1\}xi​∈{0,…,d−1}.

  • A unitary VVV is SU(d)-invariant if [V,U⊗n]=0[V,U^{\otimes n}]=0[V,U⊗n]=0 for every U∈SU(d)U\in\mathrm{SU}(d)U∈SU(d) (Eq. (1)).
  • VVV is 2-local on qudits a,ba,ba,b if V=Wab⊗IrestV=W_{ab}\otimes\mathbb I_{\text{rest}}V=Wab​⊗Irest​.
  • V2\mathcal V_2V2​ is the group generated by finite products of 2-local SU(d)-invariant unitaries.
  • P(σ)\mathbf P(\sigma)P(σ) is the permutation operator of σ∈Sn\sigma\in S_nσ∈Sn​, and Pab\mathbf P_{ab}Pab​ is the swap of qudits a,ba,ba,b.

For L≤min⁡{n,d−1}L\le\min\{n,d-1\}L≤min{n,d−1}, the vector (⋀m=1L∣m⟩)⊗∣0⟩⊗(n−L)\big(\bigwedge_{m=1}^L|m\rangle\big)\otimes|0\rangle^{\otimes(n-L)}(⋀m=1L​∣m⟩)⊗∣0⟩⊗(n−L) antisymmetrizes the levels 1,…,L1,\dots,L1,…,L over the first LLL qudits with weight 1/L!1/\sqrt{L!}1/L!​ (Eq. (40)). The subspace Hcomp\mathcal H_{\mathrm{comp}}Hcomp​ is the span of all permutations of these vectors (Eq. (42)), and Πcomp\Pi_{\mathrm{comp}}Πcomp​ is the orthogonal projector onto it.

For an operator AAA on one qudit, AiA_iAi​ is AAA acting on qudit iii. Let Qij=(Ii−∣0⟩⟨0∣i)∣0⟩⟨0∣jQ_{ij}=(\mathbb I_i-|0\rangle\langle0|_i)|0\rangle\langle0|_jQij​=(Ii​−∣0⟩⟨0∣i​)∣0⟩⟨0∣j​. The map Ω\OmegaΩ sends an operator ρ\rhoρ on the qudits to the n×nn\times nn×n matrix

Ω[ρ]=∑i,j=1nΩij[ρ] ∣i⟩⟨j∣,Ωij[ρ]={Tr(ΠcompρΠcomp PijQij)i≠j,Tr(ΠcompρΠcomp (Ii−∣0⟩⟨0∣i))i=j\Omega[\rho]=\sum_{i,j=1}^n\Omega_{ij}[\rho]\,|i\rangle\langle j|,\qquad \Omega_{ij}[\rho]=\begin{cases}\mathrm{Tr}\big(\Pi_{\mathrm{comp}}\rho\Pi_{\mathrm{comp}}\,\mathbf P_{ij}Q_{ij}\big)& i\neq j,\\ \mathrm{Tr}\big(\Pi_{\mathrm{comp}}\rho\Pi_{\mathrm{comp}}\,(\mathbb I_i-|0\rangle\langle0|_i)\big)& i=j\end{cases}Ω[ρ]=i,j=1∑n​Ωij​[ρ]∣i⟩⟨j∣,Ωij​[ρ]={Tr(Πcomp​ρΠcomp​Pij​Qij​)Tr(Πcomp​ρΠcomp​(Ii​−∣0⟩⟨0∣i​))​i=j,i=j​

(Eqs. (49), (51)). On the fermionic side there are nnn sites, creation operators cj†c_j^\daggercj†​, the vacuum ∣vac⟩|\mathrm{vac}\rangle∣vac⟩, and the fermionic swap Pabf=If−(ca†−cb†)(ca−cb)\mathbf P^f_{ab}=\mathbb I^f-(c_a^\dagger-c_b^\dagger)(c_a-c_b)Pabf​=If−(ca†​−cb†​)(ca​−cb​) (Eq. (28)). Its single-particle counterpart is Eab=I−(∣a⟩−∣b⟩)(⟨a∣−⟨b∣)E_{ab}=\mathbb I-(|a\rangle-|b\rangle)(\langle a|-\langle b|)Eab​=I−(∣a⟩−∣b⟩)(⟨a∣−⟨b∣) on Cn\mathbb C^nCn (Eq. (33)). The map UfU^fUf sends P(σ)[(⋀m∣m⟩)⊗∣0⟩⊗(n−L)]\mathbf P(\sigma)\big[\big(\bigwedge_{m}|m\rangle\big)\otimes|0\rangle^{\otimes(n-L)}\big]P(σ)[(⋀m​∣m⟩)⊗∣0⟩⊗(n−L)] to ∏i=1Lcσ(i)†∣vac⟩\prod_{i=1}^L c^\dagger_{\sigma(i)}|\mathrm{vac}\rangle∏i=1L​cσ(i)†​∣vac⟩ (Eq. (41)).

Formalization targets

Goal: Theorem 2 (p. 11)

For every V∈V2V\in\mathcal V_2V∈V2​, every density operator ρ\rhoρ on nnn qudits and every positive integer lll,

Tr(Ω[VρV†]l)=Tr(Ω[ρ]l).\mathrm{Tr}\big(\Omega[V\rho V^\dagger]^l\big)=\mathrm{Tr}\big(\Omega[\rho]^l\big).Tr(Ω[VρV†]l)=Tr(Ω[ρ]l).

The statement holds for all nnn and ddd. Its content is the case l≥2l\ge 2l≥2: the case l=1l=1l=1 holds for every SU(d)-invariant unitary (Eq. (55)).

Milestones (in attack order)

  1. Eq. (5): up to a global phase, a 2-local SU(d)-invariant unitary on qudits a,ba,ba,b equals eiθPab=cos⁡θ I+isin⁡θ Pabe^{i\theta\mathbf P_{ab}}=\cos\theta\,\mathbb I+i\sin\theta\,\mathbf P_{ab}eiθPab​=cosθI+isinθPab​.
  2. Eqs. (27)–(29): Pabfcj†Pabf†=cσab(j)†\mathbf P^f_{ab}c_j^\dagger\mathbf P^{f\dagger}_{ab}=c^\dagger_{\sigma_{ab}(j)}Pabf​cj†​Pabf†​=cσab​(j)†​, Pabf∣vac⟩=∣vac⟩\mathbf P^f_{ab}|\mathrm{vac}\rangle=|\mathrm{vac}\ranglePabf​∣vac⟩=∣vac⟩, and Pabf\mathbf P^f_{ab}Pabf​ is Hermitian and unitary.
  3. Eq. (31): eiθPabfcj†e−iθPabf=e−iθ(cos⁡θ cj†+isin⁡θ cσab(j)†)e^{i\theta\mathbf P^f_{ab}}c_j^\dagger e^{-i\theta\mathbf P^f_{ab}}=e^{-i\theta}(\cos\theta\,c_j^\dagger+i\sin\theta\,c^\dagger_{\sigma_{ab}(j)})eiθPabf​cj†​e−iθPabf​=e−iθ(cosθcj†​+isinθcσab​(j)†​).
  4. Eq. (34): the same dynamics written through the single-particle unitary eiθ(Eab−I)e^{i\theta(E_{ab}-\mathbb I)}eiθ(Eab​−I).
  5. p. 9: P(σ)Πcomp=ΠcompP(σ)\mathbf P(\sigma)\Pi_{\mathrm{comp}}=\Pi_{\mathrm{comp}}\mathbf P(\sigma)P(σ)Πcomp​=Πcomp​P(σ).
  6. Eq. (41) and App. C5: UfU^fUf satisfies (41) and is an isometry on Hcomp\mathcal H_{\mathrm{comp}}Hcomp​.
  7. Eq. (44): UfeiθPabΠcomp=eiθPabfUfΠcompU^fe^{i\theta\mathbf P_{ab}}\Pi_{\mathrm{comp}}=e^{i\theta\mathbf P^f_{ab}}U^f\Pi_{\mathrm{comp}}UfeiθPab​Πcomp​=eiθPabf​UfΠcomp​.
  8. App. C7, (C42)–(C43): the qudit form (51) and the fermionic form (50) of Ω\OmegaΩ agree.
  9. Lemma 3: Ω[eiθPabρe−iθPab]=eiθEabΩ[ρ]e−iθEab\Omega[e^{i\theta\mathbf P_{ab}}\rho e^{-i\theta\mathbf P_{ab}}]=e^{i\theta E_{ab}}\Omega[\rho]e^{-i\theta E_{ab}}Ω[eiθPab​ρe−iθPab​]=eiθEab​Ω[ρ]e−iθEab​, and Ω\OmegaΩ is completely positive.

Significance

Theorem 2 gives an infinite family of polynomial invariants of the state, Tr(Ω[ρ]l)\mathrm{Tr}(\Omega[\rho]^l)Tr(Ω[ρ]l) for l=1,2,…l=1,2,\dotsl=1,2,…. Together these fix the spectrum of Ω[ρ]\Omega[\rho]Ω[ρ], so every Rényi entropy of the single-particle density operator Ω[ρ]/Tr Ω[ρ]\Omega[\rho]/\mathrm{Tr}\,\Omega[\rho]Ω[ρ]/TrΩ[ρ] is conserved. Already for l=2l=2l=2 the law is violated by SU(d)-invariant Hamiltonians with 3-local terms (p. 11 and §IV D). This shows that, for d≥3d\ge3d≥3, 2-local SU(d)-invariant gates are not universal among SU(d)-invariant unitaries, even up to relative phases, and that 3-local interactions can be detected from the dynamics of Ω\OmegaΩ. For d=2d=2d=2 the laws hold for all SU(2)-invariant unitaries.

The result is proved in the paper. As far as a search of the platform shows, it has not been formalized. A formalization adds machine-checked versions of the qudit–fermion correspondence of §IV B, including the isometry UfU^fUf and the intertwining relation (44), and of the free-fermion form of the swap dynamics. These are statements about finite-dimensional matrices, so the whole development stays inside Mathlib's linear algebra.

Difficulty

The obvious route is to show that each generator acts on Ω[ρ]\Omega[\rho]Ω[ρ] by conjugation with an n×nn\times nn×n unitary, and then to induct over products. The difficulty is the generator step. The definition (51) of Ω\OmegaΩ involves the projector Πcomp\Pi_{\mathrm{comp}}Πcomp​ onto a span of antisymmetrized vectors, and nothing in (51) shows directly why conjugating ρ\rhoρ by eiθPabe^{i\theta\mathbf P_{ab}}eiθPab​ should conjugate Ω[ρ]\Omega[\rho]Ω[ρ] by eiθEabe^{i\theta E_{ab}}eiθEab​. The covariance becomes visible only after Hcomp\mathcal H_{\mathrm{comp}}Hcomp​ is identified with fermionic Fock sectors, where the swap becomes a quadratic, particle-number-preserving Hamiltonian. That identification needs care with the signs of the fermionic creation operators and with the ordering of products. A second obstacle is the characterization of the generators (Eq. (5)). It rests on the commutant of {U⊗U:U∈SU(d)}\{U\otimes U : U\in\mathrm{SU}(d)\}{U⊗U:U∈SU(d)} being spanned by I\mathbb II and the swap, a Schur–Weyl statement for two qudits that Mathlib does not provide.

Formalization scope

Operators on the qudits are matrices indexed by Fin n → Fin d, with sites and levels 0-based and [NeZero d] assumed so that ∣0⟩|0\rangle∣0⟩ exists. Fock-space operators are matrices indexed by Finset (Fin n), the set of occupied sites. The creation operator uses the Jordan–Wigner sign (−1)∣{k∈T:k<j}∣(-1)^{|\{k\in T:k<j\}|}(−1)∣{k∈T:k<j}∣, the encoding of the public definition QAlgorithms_Papers_Independent_Next46_P23, copied rather than imported.

The following conventions are fixed:

  • P(σ)∣y⟩=∣y∘σ−1⟩\mathbf P(\sigma)|y\rangle=|y\circ\sigma^{-1}\rangleP(σ)∣y⟩=∣y∘σ−1⟩, the representation convention the paper uses in Eq. (30) and App. C5. Eq. (9) as printed describes P(σ−1)\mathbf P(\sigma^{-1})P(σ−1), and under it the map of Eq. (41) is not well defined. All other objects coincide under the two conventions.
  • Exponentials of involutions are written in the closed form cos⁡θ I+isin⁡θX\cos\theta\,\mathbb I+i\sin\theta XcosθI+isinθX of Eq. (5), and θ\thetaθ ranges over [0,2π)[0,2\pi)[0,2π) as in the paper.
  • Πcomp\Pi_{\mathrm{comp}}Πcomp​ is the matrix of Mathlib's orthogonal projection onto Hcomp⊆\mathcal H_{\mathrm{comp}}\subseteqHcomp​⊆ EuclideanSpace ℂ (Fin n → Fin d).
  • UfU^fUf is an explicit linear map defined on the whole space. It sends the basis state with ∣m⟩|m\rangle∣m⟩ on site p(m)p(m)p(m), m=1,…,Lm=1,\dots,Lm=1,…,L, to 1L!cp(1)†⋯cp(L)†∣vac⟩\frac1{\sqrt{L!}}c^\dagger_{p(1)}\cdots c^\dagger_{p(L)}|\mathrm{vac}\rangleL!​1​cp(1)†​⋯cp(L)†​∣vac⟩, and all other basis states to 000.
  • Complete positivity is the published QAlgorithms.Entanglement.IsCompletelyPositive.

The following trivializing formalizations are ruled out:

  • Ω\OmegaΩ is not identically zero: the normalization 1/L!1/\sqrt{L!}1/L!​ and the range L≤min⁡{n,d−1}L\le\min\{n,d-1\}L≤min{n,d−1} are as printed, and Hcomp≠0\mathcal H_{\mathrm{comp}}\neq 0Hcomp​=0 is checked.
  • V2\mathcal V_2V2​ is the group generated by all 2-local SU(d)-invariant unitaries, defined literally on p. 3. It is neither the generating set of Eq. (6) nor the group of all SU(d)-invariant unitaries, for which the statement is false when d≥3d\ge3d≥3.
  • The goal uses the qudit form (51) of Ω\OmegaΩ, not the fermionic form (50).

A complete development needs:

  • the two-qudit commutant of U⊗UU\otimes UU⊗U;
  • the CAR algebra on Finset Fock space;
  • the orthonormality of the antisymmetrized vectors;
  • the trace identity Tr((WXW†)l)=Tr(Xl)\mathrm{Tr}((WXW^\dagger)^l)=\mathrm{Tr}(X^l)Tr((WXW†)l)=Tr(Xl).

The Fock-space and permutation-operator lemmas can be reused for other qudit–fermion and Schur–Weyl statements. Contributions welcome: proofs of any milestone, and lemma-level infrastructure on the Fock space.

Selected references

  • I. Marvian, H. Liu, A. Hulse, Qudit circuits with SU(d) symmetry: Locality imposes additional conservation laws, arXiv:2105.12877v2, 2022. https://arxiv.org/abs/2105.12877
  • I. Marvian, Restrictions on realizable unitary operations imposed by symmetry and locality, Nature Physics 18, 283–289, 2022. https://doi.org/10.1038/s41567-021-01464-0
  • I. Marin, L'algèbre de Lie des transpositions, Journal of Algebra 310, 742–774, 2007. https://doi.org/10.1016/j.jalgebra.2006.08.018
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Computation of Dynamic Equilibria in Series-Parallel Networks: The Thin-Flow Label Function of a Series-Parallel Network Has at Most 2|A′| − |A*| − |V| + 1 BreakpointsResearch Paper

Motivation

In the fluid queuing model (Vickrey's model) of flows over time, a continuum of infinitesimal particles travels from a source sss to a sink ttt through a network whose arcs have capacities and transit times. Each particle picks a route that minimizes its own arrival time, and a dynamic equilibrium (a Nash flow over time) is a flow in which no particle can arrive earlier by deviating. Dynamic equilibria are a basic model of congestion in road traffic and communication networks.

Koch and Skutella (2011) showed that the derivatives of a dynamic equilibrium are normalized thin flows with resetting, and Cominetti, Correa and Larré (2015) proved that such thin flows always exist, which gives existence of equilibria. Computing a thin flow, however, was known to be efficient only in the two extreme cases where no arc or every arc is resetting. Kaiser (2022) casts thin flows as a linear complementarity problem, studies how they depend on the flow value, and shows that on two-terminal series-parallel networks the whole family of thin flows, for all flow values at once, can be computed in polynomial time. The key quantitative fact behind that algorithm is a bound on the number of breakpoints of the thin-flow labels as a function of the flow value. This mission formalizes that bound and the chain of results it rests on.

  • 2011: Koch and Skutella characterize the derivatives of Nash flows over time by thin flows with resetting.
  • 2015: Cominetti, Correa and Larré prove existence of normalized thin flows with resetting and of dynamic equilibria for LpL^pLp inflow rates.
  • 2020/2022: Kaiser gives the LCP formulation, the parametric analysis and the series-parallel algorithm.

Setting

A network is a finite directed multigraph with vertex set VVV, arc set A′A'A′ and two vertices s≠ts \ne ts=t. It is a shortest path graph if A′A'A′ is acyclic and every vertex is reachable from sss. Fix a set A∗⊆A′A^* \subseteq A'A∗⊆A′ of resetting arcs and capacities νa>0\nu_a > 0νa​>0. A static sss–ttt-flow of value ν0′\nu'_0ν0′​ is a vector x′≥0x' \ge 0x′≥0 on the arcs that is conserved at every vertex other than s,ts, ts,t and has net outflow ν0′\nu'_0ν0′​ at sss.

Along an arc a=(v,w)a = (v,w)a=(v,w) a label is propagated by

ϱa(ℓv′,xa′)={max⁡{ℓv′,xa′/νa}a∉A∗,xa′/νaa∈A∗.\varrho^a(\ell'_v, x'_a) = \begin{cases}\max\{\ell'_v, x'_a/\nu_a\} & a \notin A^*,\\ x'_a/\nu_a & a \in A^*.\end{cases}ϱa(ℓv′​,xa′​)={max{ℓv′​,xa′​/νa​}xa′​/νa​​a∈/A∗,a∈A∗.​

Labels ℓ′∈R≥0V\ell' \in \mathbb R^V_{\ge 0}ℓ′∈R≥0V​ correspond to the flow x′x'x′ if ℓw′=min⁡a=(v,w)ϱa(ℓv′,xa′)\ell'_w = \min_{a = (v,w)} \varrho^a(\ell'_v, x'_a)ℓw′​=mina=(v,w)​ϱa(ℓv′​,xa′​) for every w≠sw \ne sw=s and ℓw′=ϱa(ℓv′,xa′)\ell'_w = \varrho^a(\ell'_v, x'_a)ℓw′​=ϱa(ℓv′​,xa′​) on every arc with xa′>0x'_a > 0xa′​>0; such an x′x'x′ is a normalized thin flow with resetting (Definition 4).

The label function ϱG′\varrho^{G'}ϱG′ maps each flow value ν0′≥0\nu'_0 \ge 0ν0′​≥0 to the corresponding labels, with label 111 at sss, of a normalized thin flow of value ν0′\nu'_0ν0′​. A breakpoint of ϱG′\varrho^{G'}ϱG′ is a value ν0′>0\nu'_0 > 0ν0′​>0 around which some component of ϱG′\varrho^{G'}ϱG′ is not affine.

A two-terminal series-parallel multigraph is built from single arcs s→ts \to ts→t by series composition G1∗G2G_1 * G_2G1​∗G2​ (sink of G1G_1G1​ glued to source of G2G_2G2​) and parallel composition G1∥G2G_1 \parallel G_2G1​∥G2​ (sources glued, sinks glued).

Formalization targets

Goal: Theorem 31

For a two-terminal series-parallel multigraph G′=(V,A′)G' = (V, A')G′=(V,A′), any A∗⊆A′A^* \subseteq A'A∗⊆A′ and any capacities ν>0\nu > 0ν>0: the label function ϱG′\varrho^{G'}ϱG′ exists, is continuous on [0,∞)[0,\infty)[0,∞), has finitely many breakpoints, and

#{breakpoints of ϱG′}≤2∣A′∣−∣A∗∣−∣V∣+1.\#\{\text{breakpoints of } \varrho^{G'}\} \le 2|A'| - |A^*| - |V| + 1 .#{breakpoints of ϱG′}≤2∣A′∣−∣A∗∣−∣V∣+1.

Milestones

The milestones follow the paper's proof path.

  • Theorem 6. Normalized thin flows are exactly the solutions of a linear complementarity problem (LCP) that also satisfy a normalization constraint.
  • Lemma 7 and Corollary 8. A normalization map π\piπ turns every LCP solution into a thin flow.
  • Lemmas 11, 12 and 9. The LCP matrix has non-negative principal minors, via the factorization L=BD(B+)⊤L = BD(B^+)^\topL=BD(B+)⊤ of weighted Laplacians.
  • Theorem 13 (existence). A thin flow exists for every flow value and every label at sss.
  • Theorem 14 and Corollary 15. Labels are monotone in the flow value and the label at sss, and they are unique.
  • Proposition 17. ϱG′\varrho^{G'}ϱG′ is continuous and piecewise linear.
  • Lemma 18. Scaling and monotonicity of ϱG′\varrho^{G'}ϱG′.
  • Lemmas 29 and 30. Series composition gives n≤n1+n2n \le n_1 + n_2n≤n1​+n2​ breakpoints, and parallel composition gives n≤n1+n2+1n \le n_1 + n_2 + 1n≤n1​+n2​+1.

Significance

The bound is what makes the recursive computation of ϱG′\varrho^{G'}ϱG′ along a series-parallel decomposition run in time polynomial in the size of the network. Each composition step is linear in the number of pieces, and Theorem 31 keeps the number of pieces linear in ∣A′∣|A'|∣A′∣. Combined with the paper's §5, the result computes dynamic equilibria in series-parallel networks for piecewise constant, and more generally right-monotone, inflow rates. For general graphs the complexity of computing a thin flow with resetting is open: the problem lies in PPAD, and no polynomial algorithm is known. The bound is attained already for a single non-resetting arc, whose label at ttt is max⁡{1,ν0′/νa}\max\{1, \nu'_0/\nu_a\}max{1,ν0′​/νa​}.

The results are proved in the paper. None of them has been formalized: there is no machine-checked theory of flows over time, thin flows or directed series-parallel graphs. A formalization adds three things. It gives a checked LCP formulation of thin flows, which is reusable for any equilibrium computation in this model. It gives a checked parametric analysis (existence, uniqueness, monotonicity and piecewise linearity of the labels). And it gives a complete account of the counting argument for parallel composition, which the paper extends from the sink's label to the whole label vector only in outline ("Repeating the counting more carefully…").

Difficulty

Existence (Theorem 13) is not elementary. It combines a principal-minor computation for a block matrix with a theorem from LCP theory: a P0P_0P0​-matrix whose LCP has only the trivial solution at zero data has a solution for every right-hand side. Mathlib has neither. Piecewise linearity (Proposition 17) likewise uses that solution sets of an LCP are finite unions of polyhedra.

The breakpoint count is subtle in the parallel case. Splitting the flow ν0′=ν1′+ν2′\nu'_0 = \nu'_1 + \nu'_2ν0′​=ν1′​+ν2′​ between the two parts is generally not unique, so ϱG′\varrho^{G'}ϱG′ is not simply a composition of ϱG1′\varrho^{G'_1}ϱG1′​ and ϱG2′\varrho^{G'_2}ϱG2′​. The proof constructs a piecewise linear selection of the split and counts where its pieces can change. A tempting shortcut is to bound only the breakpoints of the sink's label ϱtG′\varrho^{G'}_tϱtG′​. That is weaker than what is claimed, which is a bound for the entire label vector.

Formalization scope

  • Representation.
    • Networks are bundled finite multigraphs (Net) with arc types and tail/head maps, so parallel arcs are first-class.
    • A∗A^*A∗ is a Finset of arcs and capacities are real with ν>0\nu > 0ν>0.
    • The minimum in Definition 4 is IsLeast, never sInf.
    • The two-terminal series-parallel graphs are the graphs T.toNet of terms T : SPTerm built from arc, series and par. Every member of Definition 28's class is isomorphic to such a graph, and all quantities here are isomorphism-invariant.
  • Label functions. Statements about ϱG′\varrho^{G'}ϱG′ are made about every function with its defining property: value ν0′≥0\nu'_0 \ge 0ν0′​≥0, corresponding labels, label exactly 111 at sss. By Corollary 15 such a function is unique on [0,∞)[0,\infty)[0,∞). The goal also asserts that one exists, so the bound cannot hold vacuously because no label function exists.
  • Breakpoints. A breakpoint is a point ν0′>0\nu'_0 > 0ν0′​>0 near which some component is not affine. They are counted for the whole vector, with Set.encard in Lemmas 29–30 and with Set.ncard plus finiteness in the goal.
  • Arithmetic. The bound 2∣A′∣−∣A∗∣−∣V∣+12|A'| - |A^*| - |V| + 12∣A′∣−∣A∗∣−∣V∣+1 is computed in Z\mathbb ZZ.
  • The normalization π\piπ. It is computed by ∣V∣|V|∣V∣ sweeps of its update rule, which equals the topological-order recursion on acyclic graphs.
  • Additions relative to the page.
    • s≠ts \ne ts=t is added as a hypothesis in the flow statements of §4. It is the standing assumption of §2.
    • Lemma 11 assumes no self-loops, since the identity fails for a self-loop.
    • Lemma 18 (i) uses ℓ0′>0\ell'_0 > 0ℓ0′​>0; at ℓ0′=0\ell'_0 = 0ℓ0′​=0 the printed claim divides by zero and fails.
    • Lemma 18 adds the capacities, which the page omits.
    • In Lemmas 29–30 the parts inherit A∗A^*A∗ and ν\nuν by restriction.
  • Not formalized. The second clause of Theorem 31, "can be computed in polynomial time", is not formalized, and neither is Corollary 32: Mathlib has no cost model for real-number algorithms. The dynamic model of §§2–3 and §5 (inflow rates, queues, Theorem 24) is outside this mission.

A complete development needs:

  • an LCP theory for P0P_0P0​-matrices (existence, and piecewise linearity of parametric solutions);
  • Gershgorin-type bounds for diagonally dominant matrices;
  • elementary combinatorics of acyclic multigraphs.

The LCP layer and the network and series-parallel layer are reusable beyond this mission. Contributions to either are welcome, as are proofs of the elementary milestones (Lemma 7, Lemma 11, Theorem 14, Corollary 15) independently of the rest.

Selected references

  • M. Kaiser, Computation of Dynamic Equilibria in Series-Parallel Networks, Mathematics of Operations Research, 2022; preprint arXiv:2002.11428v2 (2020). https://arxiv.org/abs/2002.11428
  • R. Koch and M. Skutella, Nash equilibria and the price of anarchy for flows over time, Theory of Computing Systems 49 (2011). https://doi.org/10.1007/s00224-010-9299-y
  • R. Cominetti, J. Correa and O. Larré, Dynamic equilibria in fluid queueing networks, Operations Research 63 (2015). https://doi.org/10.1287/opre.2015.1348
  • R. W. Cottle, J.-S. Pang and R. E. Stone, The Linear Complementarity Problem, SIAM Classics in Applied Mathematics, 2009. https://doi.org/10.1137/1.9780898719000
17 thms2 active usersReviewed
AlgebraCombinatoricsRepresentation Theory·Captain: mikedeng1

Supersymmetric Polynomials and the Center of the Walled Brauer Algebra: When B_{r,s}(δ) Is Semisimple, Supersymmetric Polynomials in the Jucys–Murphy Elements Generate Its CenterResearch Paper

Motivation

The walled Brauer algebra Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is the centralizer algebra of mixed Schur–Weyl duality: for δ=n\delta=nδ=n it acts on the mixed tensor space V⊗r⊗(V∗)⊗sV^{\otimes r}\otimes (V^*)^{\otimes s}V⊗r⊗(V∗)⊗s of V=CnV=\mathbb C^nV=Cn and commutes with gln\mathfrak{gl}_ngln​, and for δ=m−n\delta=m-nδ=m−n it plays the same role for the general linear supergroup GL(m∣n)GL(m|n)GL(m∣n). Its representation theory has been studied through cellular structures and blocks (Cox–De Visscher–Doty–Martin 2008), Khovanov arc algebras (Brundan–Stroppel 2012) and cyclotomic quotients (Sartori–Stroppel 2015).

For the group algebra CSn\mathbb C\mathfrak S_nCSn​ of the symmetric group there is a classical description of the center: it consists of the symmetric polynomials in the Jucys–Murphy elements Lk=∑j<k(j,k)L_k=\sum_{j<k}(j,k)Lk​=∑j<k​(j,k) (Jucys 1974, Murphy 1983). Jung and Kim (arXiv:1508.06469v2) prove the walled analogue: when Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is semisimple, its center is generated by the supersymmetric polynomials in its Jucys–Murphy elements. This mission formalizes that theorem and the chain of results leading to it.

Timeline. Jucys (1974) and Murphy (1981, 1983) describe the center of CSn\mathbb C\mathfrak S_nCSn​ through Jucys–Murphy elements. Stembridge (1985) characterizes supersymmetric polynomials and shows that the power sums generate them. Cox, De Visscher, Doty and Martin (2008) give the cellular structure of Br,s(δ)B_{r,s}(\delta)Br,s​(δ), its blocks in characteristic zero and a semisimplicity criterion. Brundan and Stroppel (2012) prove that the central element zr,sz_{r,s}zr,s​ (essentially L1+⋯+Lr+sL_1+\dots+L_{r+s}L1​+⋯+Lr+s​) acts on cell modules by a content sum. Jung and Kim (2015, revised 2017) prove the generation theorem for all supersymmetric polynomials.

Setting

Fix integers r,s≥0r,s\ge0r,s≥0 and δ∈C\delta\in\mathbb Cδ∈C. An (r,s)(r,s)(r,s)-walled Brauer diagram is a pairing of 2(r+s)2(r+s)2(r+s) vertices, r+sr+sr+s on top and r+sr+sr+s on the bottom, with a wall between positions rrr and r+1r+1r+1, such that vertical edges do not cross the wall and horizontal edges do. Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is the complex vector space with these diagrams as basis; two diagrams are multiplied by stacking them and replacing each closed loop by a factor δ\deltaδ.

For vertices a≠ba\ne ba=b on the same side of the wall, (a,b)(a,b)(a,b) is the diagram of the transposition of aaa and bbb. For 1≤j≤r<k≤r+s1\le j\le r<k\le r+s1≤j≤r<k≤r+s, ej,ke_{j,k}ej,k​ is the diagram with a top arc and a bottom arc joining jjj and kkk and all other vertices joined straight down. The Jucys–Murphy elements (Definition 2.1) are

Lk=∑j=1k−1(j,k)(1≤k≤r),Lk=−∑j=1rej,k+∑j=r+1k−1(j,k)+δ(r<k≤r+s).L_k=\sum_{j=1}^{k-1}(j,k)\quad(1\le k\le r),\qquad L_k=-\sum_{j=1}^{r}e_{j,k}+\sum_{j=r+1}^{k-1}(j,k)+\delta\quad(r<k\le r+s).Lk​=j=1∑k−1​(j,k)(1≤k≤r),Lk​=−j=1∑r​ej,k​+j=r+1∑k−1​(j,k)+δ(r<k≤r+s).

A polynomial p∈C[x1,…,xr,y1,…,ys]p\in\mathbb C[x_1,\dots,x_r,y_1,\dots,y_s]p∈C[x1​,…,xr​,y1​,…,ys​] is supersymmetric (Definition 2.8) if it is symmetric in the xix_ixi​ and in the yjy_jyj​ separately, and the substitution xr=−y1=tx_r=-y_1=txr​=−y1​=t produces a polynomial independent of ttt. Examples are the power sums pk=∑ixik+(−1)k+1∑jyjkp_k=\sum_i x_i^k+(-1)^{k+1}\sum_j y_j^kpk​=∑i​xik​+(−1)k+1∑j​yjk​. Write Sr,s[x;y]S_{r,s}[x;y]Sr,s​[x;y] for the supersymmetric polynomials and p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) for the substitution xi↦Lix_i\mapsto L_ixi​↦Li​, yj↦Lr+jy_j\mapsto L_{r+j}yj​↦Lr+j​.

The cell modules Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ) are indexed by bipartitions λ=(λL,λR)\lambda=(\lambda^L,\lambda^R)λ=(λL,λR) with ∣λL∣=r−t|\lambda^L|=r-t∣λL∣=r−t, ∣λR∣=s−t|\lambda^R|=s-t∣λR∣=s−t, 0≤t≤min⁡(r,s)0\le t\le\min(r,s)0≤t≤min(r,s); this set is Λr,s\Lambda_{r,s}Λr,s​. The set Λ˙r,s\dot\Lambda_{r,s}Λ˙r,s​ equals Λr,s\Lambda_{r,s}Λr,s​ except when δ=0\delta=0δ=0 and r=s≠0r=s\ne0r=s=0, where (∅,∅)(\varnothing,\varnothing)(∅,∅) is removed; it indexes the simple modules. The content vector c(λ,⋅)∈Cr+sc(\lambda,\cdot)\in\mathbb C^{r+s}c(λ,⋅)∈Cr+s lists the contents of λL\lambda^LλL, then 2t2t2t zeros, then the contents of λR\lambda^RλR shifted by δ\deltaδ.

Formalization targets

Goal: Theorem 3.5

Br,s(δ) semisimple ⟹ C[p(L1,…,Lr+s):p∈Sr,s[x;y]]=Z(Br,s(δ)).B_{r,s}(\delta)\ \text{semisimple}\ \Longrightarrow\ \mathbb C\bigl[p(L_1,\dots,L_{r+s}) : p\in S_{r,s}[x;y]\bigr]=Z\bigl(B_{r,s}(\delta)\bigr).Br,s​(δ) semisimple ⟹ C[p(L1​,…,Lr+s​):p∈Sr,s​[x;y]]=Z(Br,s​(δ)).

Both inclusions are asserted. The goal fixes no constants; the hypothesis holds for all but finitely many δ\deltaδ (Proposition 1.1).

Milestones

  1. Relations among generators: Lemma 2.3 and Proposition 2.4.
  2. The LkL_kLk​ commute (Proposition 2.6); the power sums pk(L1,…,Lr+s)p_k(L_1,\dots,L_{r+s})pk​(L1​,…,Lr+s​) are central (Proposition 2.7).
  3. Stembridge's theorem, Sr,s[x;y]=C[p0,p1,… ]S_{r,s}[x;y]=\mathbb C[p_0,p_1,\dots]Sr,s​[x;y]=C[p0​,p1​,…], and its consequence, Corollary 2.9: every p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) with ppp supersymmetric is central, for every δ\deltaδ.
  4. Separation: Lemma 2.11 (generating functions), the semisimplicity criterion Proposition 1.1, and Lemma 2.12 (supersymmetric polynomials separate the content vectors).
  5. Central characters: Lemma 3.2, Proposition 3.1 and Corollary 3.3, by which f(L1,…,Lr+s)f(L_1,\dots,L_{r+s})f(L1​,…,Lr+s​) acts on Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ) as f(c(λ,1),…,c(λ,r+s))f(c(\lambda,1),\dots,c(\lambda,r+s))f(c(λ,1),…,c(λ,r+s)).
  6. Counting: Lemma 3.4 (a nonsingular evaluation matrix) and dim⁡Z(Br,s(δ))=∣Λ˙r,s∣\dim Z(B_{r,s}(\delta))=|\dot\Lambda_{r,s}|dimZ(Br,s​(δ))=∣Λ˙r,s​∣ in the semisimple case.

Significance

The theorem gives an explicit generating set for the center of a semisimple walled Brauer algebra, parallel to the symmetric-group case. Its consequences in the paper include a description of the Gelfand–Zetlin subalgebra and formulas for primitive idempotents (§4), an alternative proof of the block classification of Cox et al. (§5), and, via the same method, the center of the quantized walled Brauer algebra (§6). Corollary 2.9 alone, valid for every δ\deltaδ, provides a supply of central elements whose action on each cell module is computed by Corollary 3.3.

The theorem is proved in the paper; no part of it is formalized. A formalization would supply machine-checked Jucys–Murphy relations for a diagram algebra built on a published, generic encoding of walled Brauer diagrams, a Lean development of supersymmetric polynomials (including Stembridge's theorem, absent from Mathlib), and a reusable dimension count for centers of semisimple algebras in terms of simple modules.

Difficulty

The inclusion of the supersymmetric polynomials in the center (Corollary 2.9) reduces to diagram relations plus Stembridge's theorem; the latter is a nontrivial statement about polynomial rings, with no counterpart in Mathlib. The reverse inclusion is the harder half. A central element is not visibly a polynomial in the LkL_kLk​: the argument must show that enough linearly independent central elements of the form p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) exist, which requires computing their scalars on every cell module (an explicit cellular computation involving the arc elements τt\tau_tτt​), separating all content vectors (where semisimplicity enters through the criterion of Cox et al.), and comparing with dim⁡Z\dim ZdimZ, which needs Wedderburn–Artin together with the classification of simple modules. Separation genuinely fails outside the semisimple range, so no argument independent of δ\deltaδ can work.

Formalization scope

The algebra, diagrams, cell modules Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ), the index sets Λr,s\Lambda_{r,s}Λr,s​ (CellIndex) and Λ˙r,s\dot\Lambda_{r,s}Λ˙r,s​ (Label) and contents are the published definitions WalledBrauer_Blocks_{Diagram, Algebra, ModuleTheory, Partitions, CellModules}, used as references. New definitions are in WalledBrauer.Center.Setting. Conventions:

  • The base field is C\mathbb CC; r,sr,sr,s are arbitrary natural numbers, including 000; δ∈C\delta\in\mathbb Cδ∈C is arbitrary.
  • Vertices are 0-based (Fin (r + s)); the paper's LkL_kLk​ is jm δ ⟨k-1, _⟩.
  • The published algebra multiplies diagrams with the left factor on top, the opposite of the paper's convention. One-sided relations are transcribed literally with the platform's product; each is the image of the paper's relation under the up–down flip, an anti-automorphism fixing every (a,b)(a,b)(a,b), ej,ke_{j,k}ej,k​, LkL_kLk​ and τt\tau_tτt​. The center, generated subalgebras, semisimplicity and central characters do not depend on the convention.
  • Polynomials are MvPolynomial (Fin r ⊕ Fin s) ℂ. The evaluation p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) is defined monomial by monomial in increasing vertex order, without assuming that the LkL_kLk​ commute; it is never routed through a commutative subalgebra.
  • The cancellation property is vacuous when r=0r=0r=0 or s=0s=0s=0. Semisimplicity is IsSemisimpleRing, the center is Subalgebra.center ℂ, "generate" is Algebra.adjoin ℂ. In Proposition 1.1, r+s−2r+s-2r+s−2 is real.
  • Lemma 2.11's equality of rational functions is stated cross-multiplied in C[z]\mathbb C[z]C[z].

Supersymmetry is defined intrinsically on polynomials, never through the algebra, so neither inclusion of the goal holds by definition; stating only ⊆\subseteq⊆ or only ⊇\supseteq⊇ as the goal is excluded.

Proofs of any milestone are welcome, as are reusable developments of supersymmetric polynomials (Stembridge's theorem, elementary supersymmetric polynomials) and of the center of a split semisimple algebra.

Selected references

  • J. H. Jung and M. Kim, Supersymmetric polynomials and the center of the walled Brauer algebra, arXiv:1508.06469v2, 2017. https://arxiv.org/abs/1508.06469
  • A. Cox, M. De Visscher, S. Doty and P. Martin, On the blocks of the walled Brauer algebra, J. Algebra 320 (2008), 169–212. https://arxiv.org/abs/0709.0851
  • J. Brundan and C. Stroppel, Gradings on walled Brauer algebras and Khovanov's arc algebra, Adv. Math. 231 (2012), 709–773. https://arxiv.org/abs/1107.0999
  • A. Sartori and C. Stroppel, Walled Brauer algebras as idempotent truncations of level 2 cyclotomic quotients, J. Algebra 440 (2015), 602–638. https://arxiv.org/abs/1411.2771
  • J. R. Stembridge, A characterization of supersymmetric polynomials, J. Algebra 95 (1985), 439–444. https://mathscinet.ams.org/mathscinet-getitem?mr=801279
  • Y. Li, Jucys–Murphy elements and centres of cellular algebras, Bull. Aust. Math. Soc. 85 (2012), 261–270. https://mathscinet.ams.org/mathscinet-getitem?mr=2891540
  • G. E. Murphy, The idempotents of the symmetric group and Nakayama's conjecture, J. Algebra 81 (1983), 258–265. https://mathscinet.ams.org/mathscinet-getitem?mr=696137
21 thms2 active usersReviewed
Functional AnalysisQuantum InformationStatistics·Captain: mikedeng1

Randomization Theorems for Quantum Channels: Equivalent Characterizations of ε-Post-Processing Deficiency of Channels via the Diamond Norm and Its DualResearch Paper

Comparison of experiments and its quantum versions

Statistical decision theory compares two experiments by asking which one is more useful: one experiment is deficient with respect to another if, in every decision problem, it achieves nearly the same payoff. The randomization criterion turns this operational comparison into a structural one: an experiment is ϵ\epsilonϵ-deficient exactly when a Markov kernel (a randomization) maps the better experiment to within ϵ\epsilonϵ of the worse one in L1L^1L1-distance. Its exact case, the Blackwell–Sherman–Stein theorem, is a standard tool in statistics and economics, and the approximate version is the basis of Le Cam's theory of comparison of experiments (Strasser 1985; Torgersen 1991).

Quantum information asks the same question for quantum devices: when can one channel be simulated from another by further processing, and how is that detected by tasks? A short timeline of the results this mission builds on:

  • 1951. Blackwell, Sherman and Stein: the exact classical criterion for finite experiments.
  • 2005. Shmaya proves a quantum version for quantum information structures (bipartite states), with completely positive maps as randomizations.
  • 2009. Chefles reformulates Shmaya's result for comparison of quantum channels.
  • 2010. Matsumoto introduces quantum decision problems (payoff operators, channels as decision rules) and proves a quantum randomization criterion by a minimax argument.
  • 2012. Buscemi obtains a quantum Blackwell–Sherman–Stein theorem for quantum statistical models; Jenčová treats quantum binary experiments.
  • 2013–2014. Jenčová develops base-section norms, a family containing the diamond norm and its dual, and proves randomization theorems for channels in which positivity is given by an arbitrary admissible family of cones (arXiv:1404.3900v1).

This mission formalizes the central result of the last paper: the randomization theorem for post-processings of channels (Theorem 3, p. 15).

Setting

All spaces are finite-dimensional. A Hilbert space is Ch\mathbb C^hCh with its standard basis and B(H)B(H)B(H) is the algebra of h×hh\times hh×h complex matrices. A C-algebra* A⊆B(H)\mathcal A\subseteq B(H)A⊆B(H) is a block-diagonal algebra ⨁kB(Hk)\bigoplus_k B(H_k)⨁k​B(Hk​) with H=⨁kHkH=\bigoplus_k H_kH=⨁k​Hk​; full matrix algebras and the diagonal (classical) algebras Dn\mathbb D_nDn​ are the extreme cases. S(A)\mathfrak S(\mathcal A)S(A) is the set of density matrices in A\mathcal AA.

L(A,B)\mathcal L(\mathcal A,\mathcal B)L(A,B) is the real space of Hermitian linear maps from A\mathcal AA to B\mathcal BB, paired with L(B,A)\mathcal L(\mathcal B,\mathcal A)L(B,A) by ⟨ϕ,ψ⟩=s(ϕ∘ψ)\langle\phi,\psi\rangle=s(\phi\circ\psi)⟨ϕ,ψ⟩=s(ϕ∘ψ), where s(χ)=∑i,j⟨i,χ(∣i⟩⟨j∣)j⟩s(\chi)=\sum_{i,j}\langle i,\chi(|i\rangle\langle j|)j\rangles(χ)=∑i,j​⟨i,χ(∣i⟩⟨j∣)j⟩ is the trace of a map on matrices.

An admissible family of positive cones P\mathcal PP (Definition 1) assigns a closed convex cone P(H,K)\mathcal P(H,K)P(H,K) of Hermitian maps to every pair of spaces, with EB⊆P⊆PosEB\subseteq\mathcal P\subseteq PosEB⊆P⊆Pos, P∘P⊆P\mathcal P\circ\mathcal P\subseteq\mathcal PP∘P⊆P and CP∘P∘CP⊆PCP\circ\mathcal P\circ CP\subseteq\mathcal PCP∘P∘CP⊆P. Here PosPosPos, CPCPCP and EBEBEB are the positive, completely positive and entanglement-breaking maps. Examples are PosPosPos, CPCPCP, EBEBEB and the kkk-positive maps. Restricted to algebras, P(A,B)\mathcal P(\mathcal A,\mathcal B)P(A,B) is a cone in L(A,B)\mathcal L(\mathcal A,\mathcal B)L(A,B), and P∗(A,B)\mathcal P^*(\mathcal A,\mathcal B)P∗(A,B) is the dual of P(B,A)\mathcal P(\mathcal B,\mathcal A)P(B,A) under the pairing. A P\mathcal PP-channel is a trace-preserving element of P\mathcal PP; they form C(A,B)\mathcal C(\mathcal A,\mathcal B)C(A,B). ΦI,σ\Phi_{I,\sigma}ΦI,σ​ is the replacement map a↦(Tr a)σa\mapsto(\mathrm{Tr}\,a)\sigmaa↦(Tra)σ.

The two norms on L(A,B)\mathcal L(\mathcal A,\mathcal B)L(A,B) are

∥ϕ∥⋄=inf⁡α∈C(A,B)inf⁡{λ>0:−λα≤ϕ≤λα},∥ϕ∥⋄=inf⁡σ∈S(B)inf⁡{λ>0:−λΦI,σ≤∗ϕ≤∗λΦI,σ},\|\phi\|_\diamond=\inf_{\alpha\in\mathcal C(\mathcal A,\mathcal B)}\inf\{\lambda>0:-\lambda\alpha\le\phi\le\lambda\alpha\},\qquad \|\phi\|^\diamond=\inf_{\sigma\in\mathfrak S(\mathcal B)}\inf\{\lambda>0:-\lambda\Phi_{I,\sigma}\le^*\phi\le^*\lambda\Phi_{I,\sigma}\},∥ϕ∥⋄​=α∈C(A,B)inf​inf{λ>0:−λα≤ϕ≤λα},∥ϕ∥⋄=σ∈S(B)inf​inf{λ>0:−λΦI,σ​≤∗ϕ≤∗λΦI,σ​},

where ≤\le≤ and ≤∗\le^*≤∗ are the orders of P\mathcal PP and P∗\mathcal P^*P∗. For P=CP\mathcal P=CPP=CP, ∥⋅∥⋄\|\cdot\|_\diamond∥⋅∥⋄​ is the usual diamond norm.

Given channels Φ∈C(A,B)\Phi\in\mathcal C(\mathcal A,\mathcal B)Φ∈C(A,B) and Ψ∈C(A,B′)\Psi\in\mathcal C(\mathcal A,\mathcal B')Ψ∈C(A,B′), a decision algebra D\mathcal DD, decision rules α∈C(B,D)\alpha\in\mathcal C(\mathcal B,\mathcal D)α∈C(B,D) and payoff maps Γ∈P∗(D,A)\Gamma\in\mathcal P^*(\mathcal D,\mathcal A)Γ∈P∗(D,A), Ψ\PsiΨ is (ϵ,D)(\epsilon,\mathcal D)(ϵ,D)-post-processing deficient with respect to Φ\PhiΦ, written Ψ⪰ϵ,DΦ\Psi\succeq_{\epsilon,\mathcal D}\PhiΨ⪰ϵ,D​Φ, if every payoff ⟨α∘Φ,Γ⟩\langle\alpha\circ\Phi,\Gamma\rangle⟨α∘Φ,Γ⟩ achievable from Φ\PhiΦ is achievable from Ψ\PsiΨ up to ϵ∥Γ∥⋄\epsilon\|\Gamma\|^\diamondϵ∥Γ∥⋄ (Definition 3).

Formalization targets

Goal: Theorem 3 (Post-processings)

For ϵ≥0\epsilon\ge0ϵ≥0 the following are equivalent:

(i) Ψ⪰ϵ,DΦ;(ii) ∥Φ∘Γ∥⋄≤∥Ψ∘Γ∥⋄+ϵ∥Γ∥⋄  ∀ Γ∈P∗(D,A);\text{(i) } \Psi\succeq_{\epsilon,\mathcal D}\Phi;\qquad \text{(ii) } \|\Phi\circ\Gamma\|^\diamond\le\|\Psi\circ\Gamma\|^\diamond+\epsilon\|\Gamma\|^\diamond\ \ \forall\,\Gamma\in\mathcal P^*(\mathcal D,\mathcal A);(i) Ψ⪰ϵ,D​Φ;(ii) ∥Φ∘Γ∥⋄≤∥Ψ∘Γ∥⋄+ϵ∥Γ∥⋄  ∀Γ∈P∗(D,A); (iii) ∀ Γ∈L(D,A), ∀ α ∃ α′: ⟨α∘Φ,Γ⟩≤⟨α′∘Ψ,Γ⟩+2ϵ∥Γ∥⋄;(iv) ∀ α ∃ α′: ∥α∘Φ−α′∘Ψ∥⋄≤2ϵ.\text{(iii) } \forall\,\Gamma\in\mathcal L(\mathcal D,\mathcal A),\ \forall\,\alpha\ \exists\,\alpha':\ \langle\alpha\circ\Phi,\Gamma\rangle\le\langle\alpha'\circ\Psi,\Gamma\rangle+2\epsilon\|\Gamma\|^\diamond;\qquad \text{(iv) } \forall\,\alpha\ \exists\,\alpha':\ \|\alpha\circ\Phi-\alpha'\circ\Psi\|_\diamond\le2\epsilon .(iii) ∀Γ∈L(D,A), ∀α ∃α′: ⟨α∘Φ,Γ⟩≤⟨α′∘Ψ,Γ⟩+2ϵ∥Γ∥⋄;(iv) ∀α ∃α′: ∥α∘Φ−α′∘Ψ∥⋄​≤2ϵ.

Moreover, if id∈P\mathrm{id}\in\mathcal Pid∈P, then Ψ⪰ϵΦ\Psi\succeq_\epsilon\PhiΨ⪰ϵ​Φ (all decision algebras) iff Ψ⪰ϵ,BΦ\Psi\succeq_{\epsilon,\mathcal B}\PhiΨ⪰ϵ,B​Φ.

Milestones

Lemma 1 (trace property of sss); identity (1); ⟨ϕ,ΦI,σ⟩=Tr ϕ(σ)\langle\phi,\Phi_{I,\sigma}\rangle=\mathrm{Tr}\,\phi(\sigma)⟨ϕ,ΦI,σ​⟩=Trϕ(σ) (proof of Lemma 2); P∗∘P, P∘P∗⊆P∗∩CP\mathcal P^*\circ\mathcal P,\ \mathcal P\circ\mathcal P^*\subseteq\mathcal P^*\cap CPP∗∘P, P∘P∗⊆P∗∩CP (p. 8); Corollary 8 (ii) for ∥⋅∥⋄\|\cdot\|^\diamond∥⋅∥⋄; the dual formula (4) for ∥⋅∥⋄\|\cdot\|_\diamond∥⋅∥⋄​; Corollary 8 (iii) for channels; and Lemma 4, monotonicity of both norms under channels.

Significance

Theorem 3 says that a channel is approximately worse than another in every post-processing decision task exactly when every post-processing of the better channel can be approximated, in the (P\mathcal PP-)diamond norm, by a post-processing of the worse one. It contains the classical randomization criterion (classical algebras, P=Pos\mathcal P=PosP=Pos) and Matsumoto's quantum criterion (cq-channels, P=CP\mathcal P=CPP=CP) as special cases. Through the Moreover clause, it reduces deficiency over all decision algebras to a single one, the output algebra. Because P\mathcal PP is arbitrary, the same statement covers positive, kkk-positive and completely positive simulation.

The paper gives complete proofs, and the result is not open. No machine-checked version of it, of the base-section norms, or of admissible cone families exists on the platform or in Mathlib. A complete development gives a reusable, Mathlib-only layer for Hermitian maps between block algebras, their trace pairing, cone families, and the diamond norm defined relative to a cone; and a formal proof of a quantum decision-theoretic equivalence that relies on a minimax theorem.

Difficulty

The equivalence (i)⇔(ii) and the implication (iv)⇒(i) are short once the norm duality is available: Corollary 8 (ii) and (iii), which identify norms of positive elements and differences of channels with suprema of payoffs. Formalizing those duality statements is the first obstacle. They rest on the appendix theory of base sections, including the fact (Theorem 8) that ∥⋅∥⋄\|\cdot\|_\diamond∥⋅∥⋄​ and ∥⋅∥⋄\|\cdot\|^\diamond∥⋅∥⋄ are dual norms, which uses an extension theorem for positive functionals and closedness of the cones.

The step (iii)⇒(iv) is where the argument cannot be done pointwise. Condition (iii) gives, for each payoff Γ\GammaΓ separately, a decision rule α′\alpha'α′ depending on Γ\GammaΓ; condition (iv) needs one α′\alpha'α′ that works for all Γ\GammaΓ at once. Exchanging the two quantifiers requires a minimax theorem on the compact convex sets O⋄\mathcal O^\diamondO⋄ (the unit ball of ∥⋅∥⋄\|\cdot\|^\diamond∥⋅∥⋄) and C(B′,D)\mathcal C(\mathcal B',\mathcal D)C(B′,D), followed by formula (4). Compactness of C(B′,D)\mathcal C(\mathcal B',\mathcal D)C(B′,D) needs closedness of P\mathcal PP.

Formalization scope

All definitions are in one module, ChannelRandomization.PostProc.Setting, and depend only on Mathlib.

  • Dimensions are natural numbers and spaces are Cn\mathbb C^nCn. Maps are C\mathbb CC-linear maps of matrices, and Hermiticity ϕ(x∗)=ϕ(x)∗\phi(x^*)=\phi(x)^*ϕ(x∗)=ϕ(x)∗ is a separate predicate. sss is the page's sum (its real part, equal to it for Hermitian maps).
  • A C*-algebra is a block label c:{1,…,n}→Nc:\{1,\dots,n\}\to\mathbb Nc:{1,…,n}→N, standing for the matrices with xij=0x_{ij}=0xij​=0 whenever c(i)≠c(j)c(i)\ne c(j)c(i)=c(j). This is the paper's representation ⨁kB(Hk)⊆B(⨁kHk)\bigoplus_k B(H_k)\subseteq B(\bigoplus_k H_k)⨁k​B(Hk​)⊆B(⨁k​Hk​). L(A,B)\mathcal L(\mathcal A,\mathcal B)L(A,B) consists of the Hermitian maps with range in B\mathcal BB that vanish on the Hilbert–Schmidt complement of A\mathcal AA.
  • An admissible family is a structure with one cone for every pair of dimensions. "Proper" is encoded as closedness (in the pointwise topology). Pointedness and solidity follow from EB⊆P⊆PosEB\subseteq\mathcal P\subseteq PosEB⊆P⊆Pos.
  • ∥⋅∥⋄\|\cdot\|_\diamond∥⋅∥⋄​ and ∥⋅∥⋄\|\cdot\|^\diamond∥⋅∥⋄ are defined by the infima (5) and (7). The supremum forms (4) and Corollary 8 are theorems. All infima and suprema are real sInf/sSup. Their sets are nonempty and bounded when the dimensions are positive, and in dimension 0 both sides of every statement are 0.
  • Theorem 3 is stated for every admissible family, every pair of channels with a common input, every ϵ≥0\epsilon\ge0ϵ≥0 and every decision algebra, as a four-way equivalence (List.TFAE) together with the Moreover clause. "id∈P\mathrm{id}\in\mathcal Pid∈P" means that the identity of B(Cn)B(\mathbb C^n)B(Cn) lies in P\mathcal PP for every nnn.

The structure of admissible families is not vacuous: the positive maps form an instance, constructed sorry-free in a separate verification file. A formalization that defines the norms by the supremum formulas, fixes P=CP\mathcal P=CPP=CP, drops the closedness of the cones, or restricts the decision algebra D\mathcal DD to one kind proves a different statement and does not count.

Out of scope are the pre-processing theorem (Theorem 5, whose proof the paper omits as "practically the same as the proof of Theorem 3"), the cq- and qc-channel specializations of §3.2.1–3.2.3, the pointwise deficiency results, and the Choi-matrix formula of Theorem 1.

Contributions are welcome at every level: proofs of the milestones, a general Lean theory of base sections and their norms (Theorem 8, Corollary 8 in abstract form) that would serve other ordered-vector-space arguments, and alternative proofs of (iii)⇒(iv) using Mathlib's minimax theorem.

Selected references

  • A. Jenčová, Randomization theorems for quantum channels, arXiv preprint, 2014. https://arxiv.org/abs/1404.3900v1
  • A. Jenčová, Base norms and discrimination of generalized quantum channels, arXiv preprint, 2013. https://arxiv.org/abs/1308.4030
  • K. Matsumoto, A quantum version of randomization criterion, arXiv preprint, 2010. https://arxiv.org/abs/1012.2650
  • A. Chefles, The quantum Blackwell theorem and minimum error state discrimination, arXiv preprint, 2009. https://arxiv.org/abs/0907.0866
  • F. Buscemi, Comparison of quantum statistical models: equivalent conditions for sufficiency, Commun. Math. Phys. 310, 625–647, 2012. https://arxiv.org/abs/1004.3794
  • E. Shmaya, Comparison of information structures and completely positive maps, J. Phys. A 38, 9717–9727, 2005. https://arxiv.org/abs/quant-ph/0412001
  • D. Blackwell, Comparison of experiments, Proc. 2nd Berkeley Symp. Math. Stat. Probab., 93–102, 1951.
  • H. Strasser, Mathematical Theory of Statistics, de Gruyter, 1985; E. Torgersen, Comparison of Statistical Experiments, Cambridge University Press, 1991.
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